2024A&A...692A..89B


Query : 2024A&A...692A..89B

2024A&A...692A..89B - Astronomy and Astrophysics, volume 692A89 (2024/12-1)

X-Shooting ULLYSES: Massive stars at low metallicity VII. Stellar and wind properties of B supergiants in the Small Magellanic Cloud.

BERNINI-PERON M., SANDER A.A.C., RAMACHANDRAN V., OSKINOVA L.M., VINK J.S., VERHAMME O., NAJARRO F., JOSIEK J., BRANDS S.A., CROWTHER P.A., GOMEZ-GONZALEZ V.M.A., GORMAZ-MATAMALA A.C., HAWCROFT C., KUIPER R., MAHY L., MARCOLINO W.L.F., MARTINS L.P., MEHNER A., PARSONS T.N., PAULI D., SHENAR T., SCHOOTEMEIJER A., TODT H., VAN LOON J.T. (The XShootU Collaboration)

Abstract (from CDS):

Context. With the aim of understanding massive stars and their feedback in the early epochs of our Universe, the ULLYSES and XShootU collaborations collected the biggest homogeneous dataset of high-quality hot star spectra at low metallicity. Within the rich “zoo” of massive star stellar types, B supergiants (BSGs) represent an important connection between the main sequence and more extreme evolutionary stages. Additionally, lying toward the cool end of the hot star regime, determining their wind properties is crucial to gauging our expectations on the evolution and feedback of massive stars as, for instance, they are implicated in the bi-stability jump phenomenon.
Aims. Here, we undertake a detailed analysis of a representative sample of 18 Small Magellanic Cloud (SMC) BSGs within the ULLYSES dataset. Our UV and optical analysis samples early- and late-type BSGs (from B0 to B8), covering the bi-stability jump region. Our aim is to evaluate their evolutionary status and verify what their wind properties say about the bi-stability jump at a low-metallicity environment.
Methods. We used the stellar atmosphere code CMFGEN to model the UV and optical spectra of the sample BSGs as well as photometry in different bands. The optical range encodes photospheric properties, while the wind information resides mostly in the UV. Further, we compare our results with different evolutionary models, with previous determinations in the literature of OB stars, and with diverging mass-loss prescriptions at the bi-stability jump. Additionally, for the first time we provide BSG models in the SMC including X-rays.
Results. Our analysis yielded the following main results: (i) From a single-stellar evolution perspective, the evolutionary status of early BSGs appear less clear than late BSGs, which are agree reasonably well with H-shell burning models. (ii) Ultraviolet analysis shows evidence that the BSGs contain X-rays in their atmospheres, for which we provide constraints. In general, higher X-ray luminosity (close to the standard log(LX/L) ∼ -7) is favored for early BSGs, despite associated degeneracies. For later-type BSGs, lower values are preferred, log(LX/L) ∼ -8.5. (iii) The obtained mass-loss rates suggest neither a jump nor an unperturbed monotonic decrease with temperature. Instead, a rather constant trend appears to happen, which is at odds with the increase found for Galactic BSGs. (iv) The wind velocity behavior with temperature shows a sharp drop at ∼19 kK, very similar to the bi-stability jump observed for Galactic stars.

Abstract Copyright: © The Authors 2024

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

Simbad objects: 33

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Number of rows : 33
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 2dFS 163 s*b 00 36 58.2381836400 -73 23 33.167140224 13.84 14.95 15.11   15.14 O7.5Ib(f) 12 0
2 LHA 115-S 6 s*b 00 46 55.0295765376 -73 08 34.136808252 12.14 13.02 12.91   12.52 BI[e] 100 1
3 SK 13 s*b 00 47 12.2164410744 -73 06 33.111710784   12.52 12.48     B1.5Ia 83 0
4 BBB SMC 259 s*b 00 47 38.7409708152 -73 07 48.851948496   12.17 12.24     B3Ia 43 0
5 HD 5045 s*b 00 50 38.3868754296 -73 28 18.256667052   11.02 11.04     B1Ia+ 94 0
6 AzV 104 s*b 00 51 38.4279675528 -72 48 06.081643404 12.053 13.064 13.226   13.57 B0.5Ia 43 0
7 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
8 SK 68 s*b 00 57 31.7301247584 -71 19 59.269190304 11.32 11.96 12.09     B2.5Ia 38 0
9 SK 73 s*b 00 58 35.7838206672 -72 16 25.018020660 11.73 12.63 12.66   12.69 B1Iab-Ib 38 0
10 SK 76 s*b 00 58 55.6254525024 -72 32 08.467356804 11.64 12.65 12.75   12.84 BN0Ia 52 0
11 NGC 346 Cl* 00 59 04.4000 -72 10 39.000           ~ 547 0
12 SK 81 s*b 00 59 43.5064718376 -72 04 18.839976816 12.023 12.894 12.996   12.44 B2.5Ib 22 0
13 RMC 17 s*b 00 59 45.7300850520 -72 44 56.416111080   12.02 12.2     B0Ia 70 0
14 RMC 18 s*b 01 00 06.8830919184 -72 13 57.371461032   11.7 11.5     B1Ia 76 0
15 AzV 261 SB* 01 00 58.7194191624 -72 30 50.235757380 12.93 13.90 14.01   13.98 B2(Ib)e 29 0
16 SK 94 s*b 01 01 07.7622056304 -71 59 58.783358472   12.21 12.36 12.20   B1Ia 39 0
17 SK 95 s*b 01 01 09.3913651632 -72 27 28.543237812 11.47 12.48 12.61   12.67 B0.7Ia 36 0
18 SK 111 * 01 03 56.1979660536 -72 42 06.263659800 12.32 13.00 13.046 12.99 13.04 B8Iab 14 0
19 RMC 36 s*b 01 04 49.3494336384 -72 06 21.746153556 10.57 11.34 11.36     B3Ia 58 0
20 SK 150 s*b 01 13 01.8742585512 -72 45 48.441989592 11.593 12.564 12.676   11.42 B1.5Ia 41 0
21 Dachs SMC 3-10 EB* 01 13 42.4497160176 -73 17 29.516706528 12.49 13.54 13.48 13.72 13.54 O2-3V 45 0
22 SK 159 s*b 01 15 58.8782034384 -73 21 24.351532740 10.80 11.77 11.90     B0.2Ia 84 0
23 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
24 SK 179 s*b 01 28 27.9820036128 -72 46 55.559723628   12.97 13.09     B3II 12 0
25 WDG 1 s*b 01 41 42.0683863272 -73 50 38.183979624   11.86 11.84     B1.5Ia 74 0
26 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
27 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
28 * eps Ori s*b 05 36 12.81335 -01 12 06.9089 0.48 1.51 1.69 1.76 1.93 B0Ia 921 0
29 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
30 * kap Ori s*b 05 47 45.3888404 -09 40 10.577707 0.87 1.88 2.06 2.09 2.27 B0.5Ia 588 0
31 * nu. Oph PM* 17 59 01.5922136612 -09 46 25.080976810 5.20 4.33 3.34 2.64 2.16 G9IIIa 226 1
32 * 55 Cyg s*b 20 48 56.2915921440 +46 06 50.883645024 4.83 5.28 4.86 4.41 4.10 B2.5Ia 506 0
33 * 9 Cep s*b 21 37 55.2241394424 +62 04 54.990376788 4.49 5.03 4.73 4.42 4.24 B2Ib 315 0

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