2025A&A...697A..41B


Query : 2025A&A...697A..41B

2025A&A...697A..41B - Astronomy and Astrophysics, volume 697A41 (2025/5-1)

Coupling hydrodynamics with comoving frame radiative transfer III. The Wind Regime of Early-Type B Hypergiants.

BERNINI-PERON M., SANDER A.A.C., NAJARRO F., SABHAHIT G.N., PAULI D., LEFEVER R.R., VINK J.S., RAMACHANDRAN V., OSKINOVA L.M., GONZALEZ-TORA G. and SCHOSSER E.C.

Abstract (from CDS):

Context. B hypergiants (BHGs) are rare but important for our understanding of high-mass stellar evolution. While they occupy a similar parameter space as B supergiants (BSGs), some BHGs are known to be luminous blue variables (LBVs). Their spectral appearance with absorption and emission features shares similarities with the hotter Of/WNh stars. Yet, both their wind physics and their evolutionary connections are highly uncertain.
Aims. In this study, we aim to understand (i) the stellar atmospheric and wind structure, (ii) the wind-launching and wind-driving mechanisms, and (iii) the spectrum formation of early-type BHGs. As an observational prototype, we use ζ1 Sco (B1.5Ia+), which has a broad spectral coverage from the far-UV to the mid-IR regime.
Methods. Using the stellar atmosphere code PoWRHD, we calculated the first hydrodynamically consistent atmosphere model in the BHG wind regime. These models inherently connect stellar and wind properties in a self-consistent way. They also provide insights into the radiative driving of the calculated wind regimes and enable us to study the influence of clumping and X-rays on the resulting wind properties and structure.
Results. Our hydrodynamically consistent atmosphere model nicely reproduces the main spectral features of ζ1 Sco and represents a new framework of quantitative spectroscopy. The obtained mass-loss rate is higher than for BSGs of similar spectral types. However, despite the spectral morphology, the wind optical depth of BHG atmospheres is still considerably below unity, making them less of a transition type than the Of/WNh stars. To reproduce the spectrum, we need mild clumping with subsonic onset (f∞= 0.66, vcl = 5 km s–1). The wind shows a shallow-gradient velocity profile that deviates from the widely used β law. Even beneath the critical point, the wind is mainly driven by Fe III opacity.
Conclusions. Our investigation suggests that despite more mass loss, early-type Galactic BHGs have winds that are relatively similar to late-type BSGs. Their winds are not sufficiently optically thick that we would characterize them as “transition-type” stars, unlike Of/WNh, implying that emission features arise more easily in cooler than in hotter stars. The spectral BHG appearance is likely connected to atmospheric inhomogeneities already arising beneath the sonic point. To reach a spectral appearance similar to known LBVs, BHGs need to be either closer to the Eddington limit or have higher wind clumping than inferred for ζ1 Sco.

Abstract Copyright: © The Authors 2025

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

Simbad objects: 47

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Number of rows : 47
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 5045 s*b 00 50 38.3868754296 -73 28 18.256667052   11.02 11.04     B1Ia+ 94 0
2 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
3 LHA 115-S 45 s*b 01 05 56.3185112880 -72 19 44.760359424   11.44 11.47     B2Ia 47 0
4 HD 6884 s*b 01 07 18.2182685856 -72 28 03.657105156   10.32 10.2     B9Ia0ek 134 0
5 [HS80] 110A s*b 01 33 41.2375209576 +30 22 37.077649428 15.181 16.236 16.285 16.279 16.321 B1Ia 23 0
6 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
7 HD 270754 s*b 04 47 04.4509965192 -67 06 53.121123648 10.351 11.219 11.26   10.992 B1.5Ia 92 0
8 HD 268729 s*b 04 53 43.2832436568 -68 42 53.288900892 10.195 11.05 10.93   10.970 B5Ia+ 48 0
9 HD 32034 s*b 04 55 11.0851969440 -67 10 10.411470552 9.13 9.756 9.715 9.70 9.51 B9Iae 81 0
10 HD 268907 s*b 05 03 08.8162586160 -66 57 34.851132288 10.023 10.511 10.6     B5Ia 62 0
11 HD 269128 s*b 05 10 22.7893360416 -68 46 23.816621928 9.77 10.52 10.412 10.29 10.268 B2.5Ieq 113 0
12 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
13 HD 269700 s*b 05 31 52.2818122296 -68 32 38.857949016 9.71 10.56 10.54 10.38 10.38 B1.5Iaeq 92 0
14 SK -66 169 s*b 05 36 54.6614083464 -66 38 22.427577744   12.43 12.56     O9.7Ia+ 37 0
15 HD 38029B s*b 05 36 55.1865323232 -69 11 37.582606608           B1Ia+ 60 1
16 HD 269896 s*b 05 37 49.1356176384 -68 55 01.639049016 11.338 9.493 11.449 11.49   ON9.7Ia+ 102 0
17 RMC 138 sg* 05 38 36.1321603320 -69 05 57.971373360   12.07 11.74   11.45 A0Ia 34 0
18 [P93] 538 s*b 05 38 36.8574625728 -69 06 46.152663408   15.75 15.11   14.19 B0.5Ia+((n))Nwk 15 0
19 HTR 13 s*b 05 38 38.8639050936 -69 08 14.584145604 12.623 13.114 12.516 12.10 10.440 BN6Iap 22 0
20 RMC 142 s*b 05 38 42.7360833048 -69 05 42.617961852   12.11 11.82   11.59 B0Ia 39 0
21 SK -69 279 s*b 05 41 44.6553703752 -69 35 14.905767516 12.079 12.787 12.842 13.03 12.619 ON9.5Ia+ 70 0
22 * zet Pup BY* 08 03 35.04754 -40 00 11.3321 0.89 1.98 2.25 2.36 2.58 O4I(n)fp 1190 1
23 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
24 HD 80077 s*b 09 15 54.7869062472 -49 58 24.575734452 10.50 10.29 9.00 7.89   B2.5Ia+ 156 0
25 * 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
26 V* AG Car WR* 10 56 11.5781414448 -60 27 12.810673260 7.00 7.57 6.96 7.73   WN11h 649 0
27 HD 105056 s*b 12 05 49.8804411912 -69 34 22.996270632 6.57 9.07 8.74 8.45   ON9.7Iae 135 1
28 V* BP Cru HXB 12 26 37.5605188992 -62 46 13.261044684   12.482 10.803 10.304   B1Ia+ 731 0
29 WR 77f WR* 16 47 02.9772955944 -45 50 19.713734556   21.552 17.792 15.035 12.508 WNL/BIa+ 38 0
30 Cl* Westerlund 1 W 42 s*b 16 47 03.2521856424 -45 50 52.195013052         10.764 B9Ia+ 21 0
31 Cl* Westerlund 1 W 7 s*b 16 47 03.6281794392 -45 50 14.365482036   20.0 15.972 12.73 9.99 B5Ia+ 31 0
32 Cl* Westerlund 1 W 33 s*b 16 47 04.1256274968 -45 50 48.488202564   20.090 15.61 12.803 10.04 B5Ia+ 26 0
33 Cl* Westerlund 1 W 13 WR* 16 47 06.4540771320 -45 50 26.072579796   21.1 17.19 14.63 12.06 WNL/BIa+ 40 0
34 * zet01 Sco s*b 16 53 59.7271314888 -42 21 43.307334468 4.80 5.31 4.79 4.32 3.86 B1.5Ia+ 390 0
35 NAME Quintuplet Cluster OpC 17 46 13.9 -28 49 48           ~ 561 0
36 [FMM95] 3 s*b 17 46 15.240 -28 50 03.58           LBV 151 1
37 [GMC99] D6 s*b 17 46 17.982 -28 49 03.46           LBV 66 0
38 HD 168607 s*b 18 21 14.8856951904 -16 22 31.763755236 10.23 9.82 8.28 8.55   B9Ia+ 196 1
39 HD 168625 s*b 18 21 19.5484021368 -16 22 26.075142156 10.15 9.78 8.37 8.76   B8Ia+ 293 2
40 HD 169454 s*b 18 25 15.1937863728 -13 58 42.309359544 7.39 7.61 6.71 5.82 5.13 B1Ia+ 359 1
41 HD 173010 s*b 18 43 29.7070060440 -09 19 12.606116772 9.64 9.866 9.207 9.54   O9.7Ia+ 49 1
42 HD 183143 s*b 19 27 26.5636061496 +18 17 45.193019136 8.25 8.08 6.86 5.74 4.79 B7Ia+ 464 0
43 HD 190603 s*b 20 04 36.1742825304 +32 13 06.953333016 5.73 6.19 5.65 5.13 4.71 B1.5Ia+ 357 0
44 * 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
45 Schulte 12 s*b 20 32 40.9572199728 +41 14 29.279036940 16.1 14.45 11.702     B3-4Ia+ 453 0
46 HD 199478 s*b 20 55 49.8039729168 +47 25 03.564093468 5.79 6.12 5.64 5.16 4.78 B7Ia 231 0
47 NAME Local Group GrG ~ ~           ~ 9325 0

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