2012ApJ...751L..34V


Query : 2012ApJ...751L..34V

2012ApJ...751L..34V - Astrophys. J., 751, L34 (2012/June-1)

The transition mass-loss rate: calibrating the role of line-driven winds in massive star evolution.

VINK J.S. and GRAFENER G.

Abstract (from CDS):

A debate has arisen regarding the importance of stationary versus eruptive mass loss for massive star evolution. The reason is that stellar winds have been found to be clumped, which results in the reduction of unclumped empirical mass-loss rates. Most stellar evolution models employ theoretical mass-loss rates which are already reduced by a moderate factor of ≃2-3 compared to non-corrected empirical rates. A key question is whether these reduced rates are of the correct order of magnitude, or if they should be reduced even further, which would mean that the alternative of eruptive mass loss becomes necessary. Here we introduce the transition mass-loss rate {dot}Mtrans between O and Wolf-Rayet stars. Its novelty is that it is model independent. All that is required is postulating the spectroscopic transition point in a given data set, and determining the stellar luminosity, which is far less model dependent than the mass-loss rate. The transition mass-loss rate is subsequently used to calibrate stellar wind strength by its application to the Of/WNh stars in the Arches cluster. Good agreement is found with two alternative modeling/theoretical results, suggesting that the rates provided by current theoretical models are of the right order of magnitude in the ∼50 M☉ mass range. Our results do not confirm the specific need for eruptive mass loss as luminous blue variables, and current stellar evolution modeling for Galactic massive stars seems sound. Mass loss through alternative mechanisms might still become necessary at lower masses, and/or metallicities, and the quantification of alternative mass loss is desirable.

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Journal keyword(s): stars: early-type - stars: evolution - stars: mass-loss - stars: winds, outflows

Simbad objects: 24

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Number of rows : 24
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 92740 WR* 10 41 17.5158425712 -59 40 36.895992960 5.68 6.50 6.42 7.38   WN7h+O9III-V 426 0
2 * eta Car s*b 10 45 03.545808 -59 41 03.95124 6.37 7.03 6.48 6.123 4.41 LBV 2543 0
3 [BSP2001] 30 Em* 17 45 50.08 -28 49 26.1           O4-6If 20 0
4 WR 102ad WR* 17 45 50.22 -28 49 21.9           WN8-9 27 0
5 WR 102ae WR* 17 45 50.28 -28 49 11.4           WN9h 40 0
6 [BSP2001] 27 Em* 17 45 50.28 -28 49 17.2           O4-6I 10 0
7 [FNG2002] 20 * 17 45 50.48 -28 49 20.2           O4-6I 8 0
8 NAME Arches Cluster Cl* 17 45 50.5 -28 49 28           ~ 792 0
9 [BSP2001] 20 Em* 17 45 50.53 -28 49 18.4           O4-6I 14 0
10 WR 102ak WR* 17 45 50.54 -28 49 20.3           WN8-9 19 0
11 [BSP2001] 18 Em* 17 45 50.61 -28 49 24.0           O4-6I 11 0
12 [BSP2001] 15 Em* 17 45 50.68 -28 49 20.3           O4-6I 8 0
13 WR 102ba WR* 17 45 50.69 -28 49 22.2           WN8-9 19 0
14 [FNG2002] 40 * 17 45 50.69 -28 49 18.8           O4-6I 6 0
15 [FNG2002] 28 * 17 45 50.699 -28 49 22.21           ~ 9 0
16 [BSP2001] 13 Em* 17 45 50.72 -28 49 20.4           O4-6I 8 0
17 [BSP2001] 10 Em* 17 45 50.76 -28 49 17.5           O4-6I 9 0
18 [BSP2001] 8 Em* 17 45 50.76 -28 49 16.2           O4-6If 22 0
19 [BSP2001] 9 Em* 17 45 50.80 -28 49 18.1           O4-6I 9 0
20 [BSP2001] 7 Em* 17 45 50.82 -28 49 20.1           O4-6I 8 0
21 [BSP2001] 5 Em* 17 45 50.86 -28 49 21.5           O4-6I 7 0
22 [BSP2001] 2 Em* 17 45 51.21 -28 49 23.8           O4-6I 10 0
23 WR 102bc WR* 17 45 51.48 -28 49 25.4           WN8 19 0
24 * P Cyg s*b 20 17 47.2019733389 +38 01 58.549132671 4.66 5.24 4.82 4.28 4.02 B1-2Ia-0ep 1200 1

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