2019A&A...624A.129P


Query : 2019A&A...624A.129P

2019A&A...624A.129P - Astronomy and Astrophysics, volume 624A129-129 (2019/4-1)

The VLT-FLAMES Tarantula Survey. XXXI. Radial velocities and multiplicity constraints of red supergiant stars in 30 Doradus.

PATRICK L.R., LENNON D.J., BRITAVSKIY N., EVANS C.J., SANA H., TAYLOR W.D., HERRERO A., ALMEIDA L.A., CLARK J.S., GIELES M., LANGER N., SCHNEIDER F.R.N. and VAN LOON J.T.

Abstract (from CDS):


Aims. The incidence of multiplicity in cool, luminous massive stars is relatively unknown compared to their hotter counterparts. In this work we present radial velocity (RV) measurements and investigate the multiplicity properties of red supergiants (RSGs) in the 30 Doradus region of the Large Magellanic Cloud using multi-epoch visible spectroscopy from the VLT-FLAMES Tarantula Survey.
Methods. Exploiting the high density of absorption features in visible spectra of cool stars, we used a novel slicing technique to estimate RVs of 17 candidate RSGs in 30 Doradus from cross-correlation of the observations with model spectra.
Results. We provide absolute RV measurements (precise to better than ±1km/s) for our sample and estimate line-of-sight velocities for the Hodge 301 and SL 639 clusters, which agree well with those of hot stars in the same clusters. By combining results for the RSGs with those for nearby B-type stars, we estimate systemic velocities and line-of-sight velocity dispersions for the two clusters, obtaining estimates for their dynamical masses of log(Mdyn/M☉)=3.8±0.3 for Hodge 301, and an upper limit of log(Mdyn/M☉)<3.1±0.8 for SL 639, assuming virial equilibrium. Analysis of the multi-epoch data reveals one RV variable, potential binary candidate (VFTS 744), which is likely a semi-regular variable asymptotic giant branch star. Calculations of semi-amplitude velocities for a range of RSGs in model binary systems and literature examples of binary RSGs were used to guide our RV variability criteria. We estimate an upper limit on the observed binary fraction for our sample of 0.3; for this sample we are sensitive to maximum periods for individual objects in the range 1-10 000 days and mass ratios above 0.3 depending on the data quality. From simulations of RV measurements from binary systems given the current data, we conclude that systems within the parameter range q>0.3, logP[days]<3.5 would be detected by our variability criteria at the 90% confidence level. The intrinsic binary fraction, accounting for observational biases, is estimated using simulations of binary systems with an empirically defined distribution of parameters in which orbital periods are uniformly distributed in the 3.3<logP[days]<4.3 range. A range of intrinsic binary fractions are considered; a binary fraction of 0.3 is found to best reproduce the observed data.
Conclusions. We demonstrate that RSGs are effective extragalactic kinematic tracers by estimating the kinematic properties, including the dynamical masses of two LMC young massive clusters. In the context of binary evolution models, we conclude that the large majority of our sample consists of effectively single stars that are either currently single or in long-period systems. Further observations at greater spectral resolution or over a longer baseline, or both, are required to search for such systems.

Abstract Copyright: © ESO 2019

Journal keyword(s): binaries: spectroscopic - stars: late-type - Magellanic Clouds - galaxies: star clusters: individual: Hodge 301 - galaxies: star clusters: individual: SL 639

VizieR on-line data: <Available at CDS (J/A+A/624/A129): table2.dat tablea1.dat>

Simbad objects: 32

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Number of rows : 32
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 NGC 330 Cl* 00 56 18.55 -72 27 45.1 9.37 9.76 9.55   8.89 ~ 445 0
3 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
4 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
5 [W60] A61 s*r 05 37 13.5009609792 -69 08 34.641177540   16.31 14.17 12.92   M3Ia-Iab 16 0
6 OGLE LMC-LPV-74906 LP* 05 37 16.0784144376 -69 08 52.865216232   17.6 15.683   13.462 ~ 7 0
7 RM 1-703 s*r 05 37 35.9786637816 -69 12 29.804546160   15.68 13.732   11.695 K4Iab-Ib 21 0
8 NGC 2060 SNR 05 37 51.4466169456 -69 10 23.947092084   9.69 9.59     ~ 380 2
9 [MG73] 84 s*r 05 37 54.6397460568 -69 09 03.237511644   15.83 15.4 12.90   K4.5Iab-Ib 17 0
10 SP77 54-25 s*y 05 37 58.6665694608 -69 14 23.994668400   15.36 13.238 12.08 11.116 G5Ia 23 0
11 NAME 30 Dor Region reg 05 38.0 -69 06           ~ 261 0
12 UCAC2 1803323 * 05 38 00.5698937424 -69 09 41.519164968   16.71 15.0 14.34   ~ 10 0
13 [MG73] 90 s*r 05 38 06.6023511648 -69 03 45.146281680   16.36 14.06 12.91   K4Iab-Ib 18 0
14 H88 301 Cl* 05 38 16 -69 04.0   11.18 10.89     ~ 80 0
15 V* Z Dor s*r 05 38 16.0018297704 -69 10 11.237224368   16.798 15.037 12.49 11.367 M4Ia-Iab 43 0
16 [MG73] 93 LP* 05 38 16.6807937832 -69 04 13.956275532   16.39 13.905   11.453 M 18 0
17 2MASS J05381763-6904119 * 05 38 17.639 -69 04 11.92   15.72 13.96     ~ 19 0
18 WOH S 452 s*r 05 38 26.6986101936 -69 08 52.643186124   16.48 14.02 13.96 11.66 K5Ia-Iab 20 0
19 NGC 2070 Cl* 05 38 42 -69 06.0     7.25     ~ 406 1
20 RMC 136 Cl* 05 38 42.396 -69 06 03.36   5.81 5.40     ~ 2236 2
21 2MASS J05385119-6906411 Y*? 05 38 51.1942551336 -69 06 41.207439744   17.26 15.13   13.05 ~ 11 0
22 OGLE LMC-LPV-77177 LP* 05 39 07.1457863256 -69 01 52.872218868   17.34 15.661   13.166 M 9 0
23 2MASS J05392816-6905504 s*r 05 39 28.1781367728 -69 05 50.533755216 15.123 14.694 13.486     K:I 6 0
24 [SL63] 639 As* 05 39 39 -69 12.1   12.13 11.53     ~ 31 0
25 W61 8-4 LP* 05 39 39.4136933928 -69 11 52.047776832   16.72 14.667   11.803 M 15 0
26 W61 8-7 Ev* 05 39 41.7818080440 -69 11 31.010327160   16.8 14.670   12.087 M 18 0
27 2MASS J05395239-6909412 * 05 39 52.3921131000 -69 09 41.242502556   15.67 14.23 13.20   ~ 6 0
28 2MASS J05400700-6911415 * 05 40 07.0175128176 -69 11 41.496863316   16.87 14.92 13.68   ~ 7 0
29 NGC 2100 Cl* 05 42 07.200 -69 12 26.99           ~ 195 0
30 BMG 40 Cl* 05 44 59.099 -67 42 25.62           ~ 10 0
31 * 22 Vul SB* 20 15 30.2386386720 +23 30 32.051069712   6.192 5.176     G3Ib-II 215 0
32 V* VV Cep s*r 21 56 39.1414963149 +63 37 31.981636440 7.03 6.65 4.90 3.19 1.85 M2Ibep+B2?ep_sh 466 0

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