2015A&A...575A..50A


Query : 2015A&A...575A..50A

2015A&A...575A..50A - Astronomy and Astrophysics, volume 575A50-50 (2015/3-1)

What causes the large extensions of red supergiant atmospheres? Comparisons of interferometric observations with 1D hydrostatic, 3D convection, and 1D pulsating model atmospheres.

ARROYO-TORRES B., WITTKOWSKI M., CHIAVASSA A., SCHOLZ M., FREYTAG B., MARCAIDE J.M., HAUSCHILDT P.H., WOOD P.R. and ABELLAN F.J.

Abstract (from CDS):

This research has two main goals. First, we present the atmospheric structure and the fundamental parameters of three red supergiants (RSGs), increasing the sample of RSGs observed by near-infrared spectro-interferometry. Additionally, we test possible mechanisms that may explain the large observed atmospheric extensions of RSGs. We carried out spectro-interferometric observations of the RSGs V602 Car, HD 95687, and HD 183589 in the near-infrared K-band (1.92-2.47µm) with the VLTI/AMBER instrument at medium spectral resolution (R∼1500). To categorize and comprehend the extended atmospheres, we compared our observational results to predictions by available hydrostatic PHOENIX, available 3D convection, and new 1D self-excited pulsation models of RSGs. Our near-infrared flux spectra of V602 Car, HD 95687, and HD 183589 are well reproduced by the PHOENIX model atmospheres. The continuum visibility values are consistent with a limb-darkened disk as predicted by the PHOENIX models, allowing us to determine the angular diameter and the fundamental parameters of our sources. Nonetheless, in the case of V602 Car and HD 95686, the PHOENIX model visibilities do not predict the large observed extensions of molecular layers, most remarkably in the CO bands. Likewise, the 3D convection models and the 1D pulsation models with typical parameters of RSGs lead to compact atmospheric structures as well, which are similar to the structure of the hydrostatic PHOENIX models. They can also not explain the observed decreases in the visibilities and thus the large atmospheric molecular extensions. The full sample of our RSGs indicates increasing observed atmospheric extensions with increasing luminosity and decreasing surface gravity, and no correlation with effective temperature or variability amplitude. The location of our RSG sources in the Hertzsprung-Russell diagram is confirmed to be consistent with the red limits of recent evolutionary tracks. The observed extensions of the atmospheric layers of our sample of RSGs are comparable to those of Mira stars. This phenomenon is not predicted by any of the considered model atmospheres including available 3D convection and new 1D pulsation models of RSGs. This confirms that neither convection nor pulsation alone can levitate the molecular atmospheres of RSGs. Our observed correlation of atmospheric extension with luminosity supports a scenario of radiative acceleration on Doppler-shifted molecular lines.

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Journal keyword(s): stars: fundamental parameters - stars: individual: V602 Car - stars: individual: HD 95687 - stars: atmospheres - individual: HD 183589 - stars: supergiants

Simbad objects: 30

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Number of rows : 30
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 * omi Cet Mi* 02 19 20.79210 -02 58 39.4956   7.63 6.53 5.03   M5-9IIIe+DA 1586 0
2 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
3 * 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
4 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1169 0
5 V* RW Vel Mi* 09 20 19.4216289288 -49 31 30.538637292   10.92 8.90     M7e 38 0
6 V* X Hya Mi* 09 35 30.2667472344 -14 41 28.610073456   10.02 7.20 9.24   M7-8+e 159 0
7 V* Z Car Mi* 10 13 54.5780798664 -58 51 08.603411328     13.50     M8 28 0
8 V* W Vel Mi* 10 15 14.8298044200 -54 28 41.989481076   12.23 8.30     M9 82 0
9 * t01 Car PM* 10 36 20.5194125328 -59 33 51.817814604   6.249 5.088     K1III 34 0
10 HD 95687 s*r 11 01 35.7593300304 -61 02 55.820385276   9.130 7.90     M2Iab 46 0
11 HD 95686 * 11 01 44.8906220352 -57 34 25.642242084   11.18 10.09     K2 6 0
12 Ass Car OB 2 As* 11 08 -60.2           ~ 84 0
13 V* V602 Car s*r 11 13 29.9741868816 -60 05 28.849300980   10.68 8.815     M3Ia-Iab 57 0
14 * e Leo * 11 30 18.8933524920 -03 00 12.598924644 8.14 6.31 4.77     K3+IIIFe-0.5 153 0
15 V* BK Vir AB* 12 30 21.0136448232 +04 24 59.142255840 9.60 8.82 7.28     M7-III: 159 0
16 * gam Hya SB* 13 18 55.2976891983 -23 10 17.450424894 4.58 3.92 3.00 2.40 1.93 G8IIIa 192 0
17 * alf Sco s*r 16 29 24.45970 -26 25 55.2094 4.08 2.75 0.91 -0.64 -1.87 M1.5Iab+B2Vn 786 0
18 V* AH Sco s*r 17 11 17.0194487616 -32 19 30.714035556   10.03 8.10     M5Ia-Iab 145 0
19 V* KW Sgr s*r 17 52 00.7269495408 -28 01 20.555654448   11.45 11.00     M3Ia 94 0
20 V* VX Sgr s*r 18 08 04.0442790744 -22 13 26.600899044 11.72 9.41 6.52 3.90 2.11 M8.5Ia 622 0
21 V* UY Sct s*r 18 27 36.5281722864 -12 27 58.898573712   14.20 11.20 9.51 6.93 M4Iae 66 0
22 HD 183387 * 19 29 18.0225976176 +00 14 45.867845796   7.541 6.245     K2III 22 0
23 HD 183589 * 19 30 10.5351087360 +02 54 14.663673360   7.839 6.042     K5III 33 0
24 NGC 6803 PN 19 31 16.4826019750 +10 03 21.620200381   13.034 11.616 13.242   ~ 254 0
25 * mu. Aql PM* 19 34 05.3529921054 +07 22 44.184329526 6.87 5.63 4.45 3.55 2.94 K3-IIIbFe0.5 272 1
26 V* NU Pav LP* 20 01 44.7445781273 -59 22 33.226695613 7.97 6.66 5.13     M6III 74 0
27 V* RS Cap AB* 21 07 15.4311630672 -16 25 21.462156804   9.56 8.36     M6/7III 74 0
28 * eps Oct LP* 22 20 01.6806230015 -80 26 23.089683198   6.433 5.177     M5III 67 0
29 * bet Peg LP* 23 03 46.45746 +28 04 58.0336 6.05 4.09 2.42 0.92 -0.40 M2.5II-III 606 1
30 * psi Peg ** 23 57 45.5265520335 +25 08 29.058895098 7.91 6.25 4.66 3.20 1.86 M3III 131 0

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