2004ApJ...615..475S


Query : 2004ApJ...615..475S

2004ApJ...615..475S - Astrophys. J., 615, 475-484 (2004/November-1)

The missing luminous blue variables and the bistability jump.

SMITH N., VINK J.S. and DE KOTER A.

Abstract (from CDS):

We discuss an interesting feature of the distribution of luminous blue variables (LBVs) on the H-R diagram, and we propose a connection with the bistability jump seen in the winds of early-type supergiants. There appears to be a deficiency of quiescent LBVs on the S Doradus instability strip at luminosities between log(L/L)≃5.6 and 5.8. The upper boundary, interestingly, is also where the temperature-dependent S Doradus instability strip intersects the bistability jump at about Teff≃21,000 K. Because of increased opacity, winds of early-type supergiants are slower and denser on the cool side of the bistability jump, and we postulate that this may trigger optically thick winds that inhibit quiescent LBVs from residing there. We conduct numerical simulations of radiation-driven winds for a range of temperatures, masses, and velocity laws at log(L/L)=5.7 to see what effect the bistability jump should have. We find that for relatively low stellar masses, the order-of-magnitude increase in the wind density at the bistability jump leads to the formation of a modest to strong pseudophotosphere that might alter a star's apparent position on the H-R diagram. The effect is strongest for LBVs approaching 10 M, where the pseudophotospheres are sufficiently extended to make an early B-type star appear as a yellow hypergiant. Thus, the proposed mechanism will be most relevant for LBVs that are post-red supergiants [curiously, the upper boundary at log(L/L)≃5.8 coincides with the upper luminosity limit for red supergiants]. Further work is obviously needed, especially with regard to a possible evolutionary connection between the ``missing'' LBVs and the most luminous red supergiants and yellow hypergiants. Specifically, yellow hypergiants such as IRC +10420 and ρ Cas occupy the same luminosity range as the missing LBVs and show apparent temperature variations at constant luminosity. If these yellow hypergiants do eventually become Wolf-Rayet stars, we speculate that they may skip the normal LBV phase, at least as far as their apparent positions on the H-R diagram are concerned.

Abstract Copyright:

Journal keyword(s): Stars: Early-Type - Stars: Evolution - Stars: Mass Loss - Stars: Variables: Other - Stars: Winds, Outflows - Stars: Supergiants

CDS comments: Fig. 1 : S61 and S119 are LHA 120-S 61 and 119 in Simbad.

Simbad objects: 29

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Number of rows : 29
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 SV* HV 4476 s*b 00 43 02.5144653408 +41 49 12.212124096 16.378 17.273 17.426 17.242 17.241 LBV 52 0
2 BASW 19 s*b 00 43 33.0861943080 +41 12 10.311568308 16.363 17.338 17.325 17.172 17.257 LBV 79 0
3 HD 5980 WR* 00 59 26.5838833944 -72 09 53.927337312   11.13 11.31   11.029 WN4+O7I: 393 1
4 [HS53] A s*y 01 32 32.8025598888 +30 30 25.003726668 20.1 19.9 19.1 18.6 17.7 F8Ia 53 0
5 [HS53] C s*b 01 33 35.1032018424 +30 36 00.286017732 15.543 16.531 16.429 16.297 16.137 LBV 67 0
6 VHK 83 s*b 01 34 10.9079108155 +30 34 37.398838840 15.13 16.09 16.07 16.164 15.89 LBV 38 1
7 NAME Romano Star WR* 01 35 09.7011882336 +30 41 57.160957560   16.5 18.04     Ofpe/WN9 53 1
8 HD 269006 s*b 05 02 07.3942092168 -71 20 13.116800076 9.93 10.60 10.55 10.43 10.38 LBV 252 0
9 V* S Dor sg* 05 18 14.3570612088 -69 15 01.149576912 9.08 10.39 10.25 9.74 9.14 Be3 378 0
10 HD 269687 WR* 05 31 25.5247745448 -69 05 38.556251700 10.86 11.78 11.87 12.05   WN11h 110 0
11 HD 269858 s*b 05 36 43.6936418088 -69 29 47.451149232   10.24 10.15 9.95 9.05 LBV 283 2
12 CPD-69 463 s*y 05 38 51.6161224200 -69 08 07.314706104 11.93 12.45 12.014     F7Ia 89 1
13 SK -69 279 Em* 05 41 44.6553703752 -69 35 14.905767516 12.079 12.787 12.842 13.03 12.619 OB 53 0
14 LHA 120-S 61 WR* 05 45 51.9388258704 -67 14 25.937264544 10.870 11.86 11.95 12.09 11.931 WN11h 86 0
15 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1104 0
16 HD 90177 s*b 10 22 53.8430096928 -59 37 28.363616256 9.16 9.66 8 8.15   LBV 326 0
17 WRAY 15-682 WR* 10 53 59.5777329720 -60 26 44.361095316   11.64 10.85 10.56   WN11h 148 3
18 V* AG Car WR* 10 56 11.5781414448 -60 27 12.810673260 7.00 7.57 6.96 7.73   WN11h 631 0
19 MR 35 s*b 11 08 40.0634208096 -60 42 51.721320060   12.33 10.20 11.66   LBV 125 0
20 Cl* Westerlund 1 W 243 s*b 16 47 07.5040736160 -45 52 29.123491188   19.873 15.730     LBV 61 0
21 [B61] 2 s*b 17 41 35.4358256400 -30 06 38.782127520   18.0 15.00 14.23 10.30 LBV_B[e]: 45 0
22 HD 168625 s*b 18 21 19.5484021368 -16 22 26.075142156 10.15 9.78 8.37 8.76   B8Ia+ 279 2
23 V* V481 Sct s*b 18 33 55.2781965336 -06 58 38.631350604           LBV_B[e]: 49 0
24 MSX6C G026.4700+00.0207 s*b 18 39 32.2472383848 -05 44 20.185351872           LBV_B 41 1
25 IRAS 18576+0341 s*b 19 00 10.89456 +03 45 47.1096           B8I 86 0
26 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 477 0
27 * 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 1177 1
28 IRAS 20298+4011 LP? 20 31 42.2846664600 +40 21 59.074415640     15.1     B:I[e] 93 0
29 * rho Cas LP* 23 54 23.0325302520 +57 29 57.774737400 7.00 5.85 4.59 3.63 2.89 G2_0 383 0

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