2010MNRAS.404.1698J


Query : 2010MNRAS.404.1698J

2010MNRAS.404.1698J - Mon. Not. R. Astron. Soc., 404, 1698-1710 (2010/June-1)

Stellar winds and mass loss from extreme helium stars.

JEFFERY C.S. and HAMANN W.-R.

Abstract (from CDS):

Extreme helium stars are very rare low-mass supergiants in a late stage of evolution. They are probably contracting to become white dwarfs following a violent phase of evolution which caused them to become hydrogen-deficient giants, possibly R CrB stars. Using the latest generation of models for spherically expanding stellar atmospheres, we set out to measure mass-loss rates for a representative fraction of these stars. We have used high-resolution ultraviolet and optical spectra, and ultraviolet, optical and near-infrared photometry from a variety of archives. Overall atmospheric parameters have mostly been taken from previous analyses and checked for consistency. Mass-loss rates were measured by fitting the P Cygni and asymmetric profiles of C, N and Si ultraviolet resonance lines and lie in the range of 10–10-10–7 M yr–1. These rates follow a Castor-type relation marking a lower limit for the mass loss from hot stars of all kinds. The mass-loss rates of the stars studied also show a strong correlation with their proximity to the Eddington limit. There is no firm evidence for variability in the stellar wind, although photospheric pulsations have been reported in many cases.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): stars: chemically peculiar - stars: evolution - stars: mass-loss

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 BD+37 442 HS* 01 58 33.4346638392 +38 34 23.842803324   9.69 9.92     sdOHe 67 0
2 2MASS J06544616-1048325 pA* 06 54 46.1643701544 -10 48 32.601721752   12.99 12.27 12.08   OB+ 19 0
3 * zet Pup BY* 08 03 35.04754 -40 00 11.3321 0.89 1.98 2.25 2.36 2.58 O4I(n)fp 1154 1
4 BD+37 1977 HS* 09 24 26.3929652664 +36 42 53.295009624   9.86 10.15     sdO 48 0
5 V* DN Leo Pu* 10 38 55.2343433712 +10 03 48.486337812   9.76 9.93     Bp 144 0
6 V* DY Cen RC* 13 25 34.0847063328 -54 14 43.129581792     12.00     C-Hd/B5-6Ie 96 0
7 V* BX Cir Pu* 14 01 36.4829811264 -66 09 56.163698820 11.79 12.62 12.58 12.75   OB+ 59 0
8 V* V821 Cen Pu* 14 14 58.6292612424 -46 17 19.294106424 9.09 9.89 9.98     (B)p 138 0
9 HD 144941 pA* 16 09 24.5513020968 -27 13 38.184011148 9.45 10.17 10.02     B8 88 1
10 V* V2205 Oph Pu* 16 28 35.3724415104 -09 19 31.849139568 9.79 10.56 10.5     B 97 0
11 * tau Sco * 16 35 52.9528530 -28 12 57.661515 1.55 2.56 2.81 2.93 3.18 B0.2V 920 0
12 V* V652 Her pA* 16 48 04.6934854032 +13 15 42.420402252   10.31 10.51     ~ 137 0
13 V* V2209 Oph Mi* 17 39 57.4732345272 -24 03 26.161800984           ~ 5 0
14 HD 160641 HS* 17 41 51.5791786632 -17 53 48.462200880 9.15 10.01 9.85 10.08 9.59 sdOC9.5II-IIIHe40 123 0
15 CD-46 11775 pA* 17 42 33.9915492936 -46 58 48.829063584   11.14 11.27     OB+ 37 0
16 2MASS J17442550-1937537 pA* 17 44 25.5054075744 -19 37 53.754611844   12.8 12.60 12.62   OB+ 21 0
17 LS IV +06 2 HS* 18 06 55.4522031744 +06 21 57.246453756   12.11 12.14 12.32   sdBC1VHe39 33 0
18 V* PV Tel s?b 18 23 14.6623123440 -56 37 44.138664012 8.60 9.20 9.30     B5?I?pec 123 0
19 LS 5121 HS* 18 43 16.6073721048 -18 31 27.933194856 12.8 13.58 13.25 13.39   sdBC0IIHe40 18 0
20 V* MV Sgr RC* 18 44 31.9665722184 -20 57 12.863610864 12.82 13.56 12.00 13.37   B2pec-Hd 105 0
21 V* V4732 Sgr Pu* 18 59 39.5771671848 -14 26 17.543500548 11.19 11.5 10.9     OB+ 36 0

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