2024A&A...683A..19G


Query : 2024A&A...683A..19G

2024A&A...683A..19G - Astronomy and Astrophysics, volume 683A19 (2024/3-1)

The effect of winds on atmospheric layers of red supergiants II. Modelling VLTI/GRAVITY and MATISSE observations of AH Sco, KW Sgr, V602 Car, CK Car, and V460 Car.

GONZALEZ-TORA G., WITTKOWSKI M., DAVIES B. and PLEZ B.

Abstract (from CDS):

Context. Mass loss plays a crucial role in the lives of massive stars, especially as the star leaves the main sequence and evolves to the red supergiant (RSG) phase. Despite its importance, the physical processes that trigger mass-loss events in RSGs are still not well understood. Recently, we showed that adding a semi-empirical wind to atmosphere models can accurately reproduce observed extensions in the atmospheres of RSGs, where the mass-loss events are taking place, particularly in the CO and water lines.
Aims. By adding a static wind to a MARCS atmospheric model, we computed synthetic observables that match new interferometric data of the RSGs AH Sco, KW Sgr, V602 Car, CK Car, and V460 Car obtained with the VLTI/MATISSE and VLTI/GRAVITY instruments between August 2022 and February 2023. We also used archival VLTI/AMBER data of KW Sgr and VLTI/GRAVITY data of AH Sco. The MATISSE wavelength range includes the SiO molecule at 4.0 μm with a spectral resolution of R ∼ 500.
Methods. The model intensities with respect to the line-of-sight angle (μ) as well as the spectra and visibilities were computed using the stellar radiative transfer code TURBOSPECTRUM. We found the best-fit model, mass-loss rate, and best-fit angular Rosseland diameter for the observations. We simultaneously matched our model to the data, covering a wavelength range of 1.8-5.0 μm, which corresponds to the K, L, and M bands.
Results. Our models reproduce the spectro-interferometric data over this wide wavelength range, including extended atmospheric layers of CO, H2O, and SiO. We obtain a range of Rosseland angular diameters between 3.0 < θRoss < 5.5 mas and a range of mass-loss rates of -6.5 < log Ṁ/M⊙ yr–1 < -4 for our five targets. In our best-fit models, the partial pressure of SiO relative to the gas pressure, PSiO/Pg, and the SiO 4.0 μm line intensity increase between 2 and 3 stellar radii. The relative intensity depends on the luminosity used for our models, since the more luminous models have a higher mass-loss rate.
Conclusions. This work further demonstrates that our MARCS+wind model can reproduce the observed physical extension of RSG atmospheres for several spectral diagnostics spanning a broad wavelength range. We reproduce both spectra and visibilities of newly obtained data as well as provide temperature and density stratifications that are consistent with the observations. With the MATISSE data, we newly include the extension of SiO layers as a precursor of silicate dust.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: atmospheres - stars: evolution - stars: fundamental parameters - stars: massive - stars: mass-loss - supergiants

Simbad objects: 26

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Number of rows : 26
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 * ups Cet PM* 02 00 00.3084712060 -21 04 40.194010210 7.45 5.58 4.02 2.76 1.72 M0III 109 0
2 * 77 Cet PM* 02 34 42.6236444496 -07 51 34.002610596   7.126 5.731     K2III 24 0
3 * 80 Cet PM* 02 36 00.0478570968 -07 49 53.745797496   7.088 5.535     M0/1III 56 0
4 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1789 0
5 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1169 0
6 HD 60228 * 07 30 30.9186521808 -54 23 57.713571348   7.503 5.941     M1III 31 0
7 * Q Car V* 07 35 39.7223031408 -52 32 01.809116484   6.318 4.920     K3III 41 0
8 * zet Vol * 07 41 49.2590323455 -72 36 21.956812196   4.977 3.944     G9IIIb 81 0
9 V* V460 Car LP* 07 59 37.5423065376 -60 35 13.423848216   6.91 5.18     M1.5IIb 97 0
10 CD-55 3254 AB* 10 17 09.8283314328 -55 55 21.127054260   11.27 8.973     M3 16 0
11 HD 89736 * 10 20 16.7155651392 -47 41 56.725799604   7.293 5.614     K5/M0III 27 0
12 HD 302821 sg* 10 23 19.4847405144 -59 32 04.566918624   10.59 9.17     A7Ie 86 1
13 V* CK Car s*r 10 24 25.3598323512 -60 11 29.042707056   9.63 7.59     M3.5Iab 63 0
14 HD 90677 * 10 26 48.9214744080 -54 52 38.302832496   7.098 5.546     K3II/III 24 0
15 HD 91056 * 10 28 52.5748022328 -64 10 20.207849736   7.11 5.27   8.65 M0III 46 0
16 HD 94683 * 10 54 29.6026095360 -61 49 35.837849784 9.61 7.73 5.90     K4III 27 0
17 HD 96442 V* 11 06 19.4986197072 -50 26 51.193148640   8.67 7.03     M1/2III 16 0
18 V* V602 Car s*r 11 13 29.9741868816 -60 05 28.849300980   10.68 8.815     M3Ia-Iab 57 0
19 HD 103859 * 11 57 25.8912318168 -61 07 24.359248344   8.98 7.31     K4III 12 0
20 * gam02 Nor PM* 16 19 50.4223079953 -50 09 19.821590813 6.27 5.10 4.02 3.24 2.66 K0III 78 0
21 * eps Sco PM* 16 50 09.8108127 -34 17 35.633735 4.61 3.45 2.29 1.43 0.83 K1III 228 0
22 HD 152636 * 16 55 57.7523286192 -33 30 24.743368368   8.12 6.32     K5III 20 0
23 V* AH Sco s*r 17 11 17.0194487616 -32 19 30.714035556   10.03 8.10     M5Ia-Iab 145 0
24 HD 159881 * 17 38 11.9881032240 -28 02 48.350675544   8.85 6.90     K5III 31 0
25 V* KW Sgr s*r 17 52 00.7269495408 -28 01 20.555654448   11.45 11.00     M3Ia 94 0
26 * nu. Oph PM* 17 59 01.5922136612 -09 46 25.080976810 5.20 4.33 3.34 2.64 2.16 G9IIIa 226 1

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