2014A&A...563A..71C


Query : 2014A&A...563A..71C

2014A&A...563A..71C - Astronomy and Astrophysics, volume 563A71-71 (2014/3-1)

The yellow hypergiant HR 5171 A: Resolving a massive interacting binary in the common envelope phase.

CHESNEAU O., MEILLAND A., CHAPELLIER E., MILLOUR F., VAN GENDEREN A.M., NAZE Y., SMITH N., SPANG A., SMOKER J.V., DESSART L., KANAAN S., BENDJOYA P., FEAST M.W., GROH J.H., LOBEL A., NARDETTO N., OTERO S., OUDMAIJER R.D., TEKOLA A.G., WHITELOCK P.A., ARCOS C., CURE M. and VANZI L.

Abstract (from CDS):

Only a few stars are caught in the very brief and often crucial stages when they quickly traverse the Hertzsprung-Russell diagram, and none has yet been spatially resolved in the mass transfer phase. We initiated long-term optical interferometry monitoring of the diameters of massive and unstable yellow hypergiants (YHG) with the goal of detecting both the long-term evolution of their radius and shorter term formation of a possible pseudo-photosphere related to proposed large mass-loss events. We observed HR5171 A with AMBER/VLTI. We also examined archival photometric data in the visual and near-IR spanning more than 60 years, as well as sparse spectroscopic data. HR5171A exhibits a complex appearance. Our AMBER data reveal a surprisingly large star for a YHG R*=1315±260R☉ (or ∼6.1AU) at the distance of 3.6±0.5kpc. The source is surrounded by an extended nebulosity, and these data also show a large level of asymmetry in the brightness distribution of the system, which we attribute to a newly discovered companion star located in front of the primary star. The companion's signature is also detected in the visual photometry, which indicates an orbital period of Porb=1304±6d. Modeling the light curve with the NIGHTFALL program provides clear evidence that the system is a contact or possibly over-contact eclipsing binary. A total current system mass of 39+40–22M☉ and a high mass ratio q≥10 is inferred for the system. The low-mass companion of HR5171A is very close to the primary star that is embedded within its dense wind. Tight constraints on the inclination and vsin i of the primary are lacking, which prevents us from determining its influence precisely on the mass-loss phenomenon, but the system is probably experiencing a wind Roche-Lobe overflow. Depending on the amount of angular momentum that can be transferred to the stellar envelope, HR5171A may become a fast-rotating B[e]/luminous blue variable/Wolf-Rayet star. In any case, HR5171A highlights the possible importance of binaries for interpreting the unstable YHGs and for massive star evolution in general.

Abstract Copyright: ∼

Journal keyword(s): techniques: high angular resolution - stars: individual: HR 5171 A - binaries: close - circumstellar matter - stars: massive - stars: mass-loss

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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 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 * l Pup sg* 07 43 48.4696146486 -28 57 17.374357218 4.06 4.09 3.93 3.68 3.50 A4Iabe 201 0
6 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4725 3
7 HD 90177 s*b 10 22 53.8430096928 -59 37 28.363616256 9.16 9.66 8 8.15   LBV 342 0
8 * 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
9 V* AG Car WR* 10 56 11.5781414448 -60 27 12.810673260 7.00 7.57 6.96 7.73   WN11h 649 0
10 * z Car * 11 06 32.4264772704 -62 25 26.810615136   5.622 4.606     G7.5III 55 0
11 * x Car cC* 11 08 35.3887658400 -58 58 30.139080572 6.07 5.09 3.83 2.86 2.27 G5_0-Ia 156 0
12 * m Cen * 13 24 00.4826883840 -64 32 08.411490672 5.85 5.35 4.52     G5IIb 52 0
13 GUM 48d HII 13 47.0 -62 35           ~ 7 0
14 HD 119796B * 13 47 09.9533726304 -62 35 15.990731772   9.64 8.45     B0Ibp: 9 1
15 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
16 * kap TrA * 15 55 29.5996908168 -68 36 10.803406644   6.202 5.097     G5Ib-II 51 0
17 * del TrA * 16 15 26.2707862589 -63 41 08.453417447   4.943 3.839     G2Ib-IIa 108 0
18 WRAY 15-1676 pA* 17 19 49.3290860880 -39 10 37.928806356     13.1     O-rich 54 1
19 HD 168625 s*b 18 21 19.5484021368 -16 22 26.075142156 10.15 9.78 8.37 8.76   B8Ia+ 293 2
20 V* RY Sct Be* 18 25 31.4771300232 -12 41 24.192361500 10.25 10.38 9.12 9.46   O9.7Ibep 311 2
21 CD-44 12736 PM* 18 36 25.9502475648 -44 18 36.907592904   10.83 10.22     G0 222 0
22 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 492 0
23 HD 185018 * 19 36 52.4545556280 +11 16 23.522333484   6.834 5.975     G0Ib-II 73 0
24 HD 208606 * 21 55 20.5949872800 +61 32 30.521867352 9.35 7.692 6.125     G8Ib 78 0
25 V* V509 Cas LP* 23 00 05.1012218544 +56 56 43.350876312 8.01 6.68 5.13 3.96 3.11 G4_0 339 0
26 * rho Cas LP* 23 54 23.0325302520 +57 29 57.774737400 7.00 5.85 4.59 3.63 2.89 G2_0 401 0

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