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Statistical analysis of intrinsic polarization, IR excess and projected rotational velocity distributions of classical Be stars
We present the results of statistical analyses of a sample of 627 Bestars. The parameters of intrinsic polarization (p*),projected rotational velocity (v sin i), and near IR excesses have beeninvestigated. The values of p* have been estimated for a muchlarger and more representative sample of Be stars (~490 objects) thanpreviously. We have confirmed that most Be stars of early spectral typehave statistically larger values of polarization and IR excesses incomparison with the late spectral type stars. It is found that thedistributions of p* diverge considerably for the differentspectral subgroups. In contrast to late spectral types (B5-B9.5), thedistribution of p* for B0-B2 stars does not peak at the valuep*=0%. Statistically significant differences in the meanprojected rotational velocities (/line{vsin i}) are found for differentspectral subgroups of Be stars in the sense that late spectral typestars (V luminosity class) generally rotate faster than early types, inagreement with previously published results. This behaviour is, however,not obvious for the III-IV luminosity class stars. Nevertheless, thecalculated values of the ratio vt/vc of the truerotational velocity, vt, to the critical velocity forbreak-up, vc, is larger for late spectral type stars of allluminosity classes. Thus, late spectral type stars appear to rotatecloser to their break-up rotational velocity. The distribution of nearIR excesses for early spectral subgroups is bi-modal, the position ofthe second peak displaying a maximum value E(V-L)~ 1 . m 3for O-B1.5 stars, decreasing to E(V-L)~0. m8 for intermediatespectral types (B3-B5). It is shown that bi-modality disappears for latespectral types (B6-B9.5). No correlations were found betweenp* and near IR excesses and between E(V-L) and vsin i for thedifferent subgroups of Be stars. In contrast to near IR excesses, arelation between p* and far IR excesses at 12 mu m is clearlyseen. A clear relation between p* and vsin i (as well asbetween p* and /line{vsin i}/vc) is found by thefact that plots of these parameters are bounded by a ``triangular"distribution of p*: vsin i, with a decrease of p*towards very small and very large vsin i (and /line{vsini}/vc) values. The latter behaviour can be understood in thecontext of a larger oblateness of circumstellar disks for the stars witha rapid rotation. From the analysis of correlations between differentobservational parameters we conclude that circumstellar envelopes forthe majority of Be stars are optically thin disks with the range of thehalf-opening angle of 10degr
| UVBY photometry of HIPPARCOS stars
Photoelectric data in the uvby system have been obtained for 367southern stars of the Hipparcos Input Catalogue. Most of the stars are Fand G main sequence and fall in the magnitude range V = 9 to 10.
| Chemical composition of open clusters. I - Fe/H from high-resolution spectroscopy
Using high-resolution spectroscopy, the abundance ratios Fe/H, C/H, andC/Fe were determined for F dwarfs in the Alpha Per, the Pleiades, andthe Hyades clusters; the UMa, Hyades, and Wolf 630 moving groups; and aselection of bright F field dwarfs. The age span of these objects rangesfrom 5 x 10 to the 7th to 2 x 10 to the 9th yr. No evidence was found ofa trend in Fe/H with age for these clusters and groups, but there wereclear differences in Fe/H among these groups, indicating intrinsicdifferences in the metal content of the local gas out of which thesegroups were formed. No evidence was found for a trend of C/H with age ofthese stellar groups, but there were cluster-to-cluster variations,implying differences in the content of carbon in the precluster gas. TheC/H cluster differences followed the same pattern as the Fe/H clusterdifferences and yield C/Fe values which are constant, and equal to thesolar value, in all the groups.
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Observation and Astrometry data
| Constellation: | つる座 |
| Right ascension: | 22h54m42.30s |
| Declination: | -46°24'48.3" |
| Apparent magnitude: | 9.356 |
| Proper motion RA: | -0.2 |
| Proper motion Dec: | 20.9 |
| B-T magnitude: | 10.186 |
| V-T magnitude: | 9.425 |
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