2017A&A...597A...9W


Query : 2017A&A...597A...9W

2017A&A...597A...9W - Astronomy and Astrophysics, volume 597A9-9 (2017/1-1)

VLTI/AMBER spectro-interferometry of the late-type supergiants V766 Cen (=HR 5171 A), σ Oph, BM Sco, and HD 206859.

WITTKOWSKI M., ARROYO-TORRES B., MARCAIDE J.M., ABELLAN F.J., CHIAVASSA A. and GUIRADO J.C.

Abstract (from CDS):

Aims. We add four warmer late-type supergiants to our previous spectro-interferometric studies of red giants and supergiants.
Methods. We measure the near-continuum angular diameter, derive fundamental parameters, discuss the evolutionary stage, and study extended atmospheric atomic and molecular layers.
Results. V766 Cen (=HR 5171 A) is found to be a high-luminosity (logL/L☉=5.8±0.4) source of effective temperature 4290±760K and radius 1490±540R☉, located in the Hertzsprung-Russell (HR) diagram close to both the Hayashi limit and Eddington limit; this source is consistent with a 40M☉ evolutionary track without rotation and current mass 27-36M☉. V766 Cen exhibits NaI in emission arising from a shell of radius 1.5RPhot and a photocenter displacement of about 0.1RPhot. It shows strong extended molecular (CO) layers and a dusty circumstellar background component. The other three sources are found to have lower luminosities of about logL/L☉=3.4-3.5, corresponding to 5-9M☉ evolutionary tracks. They cover effective temperatures of 3900K to 5300K and radii of 60-120R☉. They do not show extended molecular layers as observed for higher luminosity RSGs of our sample. BM Sco shows an unusually strong contribution by an over-resolved circumstellar dust component.
Conclusions. V766 Cen is a red supergiant located close to the Hayashi limit instead of a yellow hypergiant already evolving back toward warmer effective temperatures as discussed in the literature. Our observations of the NaI line and the extended molecular layers suggest an optically thick pseudo-photosphere at about 1.5RPhot at the onset of the wind. The stars σ Oph, BM Sco, and HD 206859 are more likely high-mass red giants instead of RSGs as implied by their luminosity class Ib. This leaves us with an unsampled locus in the HR diagram corresponding to luminosities logL/L☉∼3.8-4.8 or masses 10-13M☉, possibly corresponding to the mass region where stars explode as (type II-P) supernovae during the red supergiant stage. With V766 Cen, we now confirm that our previously found relation of increasing strength of extended molecular layers with increasing luminosities extends to double our previous luminosities and up to the Eddington limit. This might further point to steadily increasing radiative winds with increasing luminosity.

Abstract Copyright: © ESO, 2016

Journal keyword(s): techniques: interferometric - supergiants - stars: atmospheres - stars: mass-loss - stars: individual: V766 Cen - stars: individual: BM Sco

CDS comments: Calibrator star BS 4432 not identified.

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 * 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
2 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1169 0
3 HD 95687 s*r 11 01 35.7593300304 -61 02 55.820385276   9.130 7.90     M2Iab 46 0
4 V* V602 Car s*r 11 13 29.9741868816 -60 05 28.849300980   10.68 8.815     M3Ia-Iab 57 0
5 * gam Hya SB* 13 18 55.2976891983 -23 10 17.450424894 4.58 3.92 3.00 2.40 1.93 G8IIIa 192 0
6 HD 119796B * 13 47 09.9533726304 -62 35 15.990731772   9.64 8.45     B0Ibp: 9 1
7 HD 119796 s*y 13 47 10.8637122288 -62 35 22.949098944 10.24 9.05 6.80 4.74 3.54 G8Ia+ 147 0
8 HD 129624 * 14 45 18.8269487664 -51 18 53.746612488   8.04 6.43     K4III 12 0
9 * 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
10 V* AH Sco s*r 17 11 17.0194487616 -32 19 30.714035556   10.03 8.10     M5Ia-Iab 145 0
11 * sig Oph V* 17 26 30.8807335272 +04 08 25.293765444 7.39 5.82 4.31 3.22 2.46 K2II 183 0
12 V* BM Sco s*r 17 40 58.5463959480 -32 12 52.064356500 8.75 7.20 5.60     K2IbHdel1 93 0
13 V* KW Sgr s*r 17 52 00.7269495408 -28 01 20.555654448   11.45 11.00     M3Ia 94 0
14 HD 162774 V* 17 52 35.4392568576 +01 18 18.039891744   7.479 5.917     K4III 25 0
15 HD 163145 * 17 56 47.4169480680 -44 20 31.986560220   6.041 4.849     K2III 33 0
16 HD 164064 PM* 17 59 36.7622850912 -04 49 16.054844088   7.381 5.832     K5III 29 0
17 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
18 V* UY Sct s*r 18 27 36.5281722864 -12 27 58.898573712   14.20 11.20 9.51 6.93 M4Iae 66 0
19 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 492 0
20 HD 183589 * 19 30 10.5351087360 +02 54 14.663673360   7.839 6.042     K5III 33 0
21 V* NU Pav LP* 20 01 44.7445781273 -59 22 33.226695613 7.97 6.66 5.13     M6III 74 0
22 * 9 Peg V* 21 44 30.6958020785 +17 21 00.062899998 6.48 5.52 4.35 3.53 2.98 G5Ib 274 0
23 * nu. Peg PM* 22 05 40.7509642224 +05 03 30.708590796 8.08 6.28 4.84 3.77 3.01 K4III 109 0
24 * eps Oct LP* 22 20 01.6806230015 -80 26 23.089683198   6.433 5.177     M5III 67 0
25 * 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
26 * 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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