2017A&A...605A.108M


Query : 2017A&A...605A.108M

2017A&A...605A.108M - Astronomy and Astrophysics, volume 605A, 108-108 (2017/9-1)

The convective surface of the red supergiant Antares. VLTI/PIONIER interferometry in the near infrared.

MONTARGES M., CHIAVASSA A., KERVELLA P., RIDGWAY S.T., PERRIN G., LE BOUQUIN J.-B. and LACOUR S.

Abstract (from CDS):

Context. Convection is a candidate to explain the trigger of red supergiant star (RSG) mass loss. Owing to the small size of the convective cells on the photosphere, few of the characteristics of RSGs are known.
Aims. Using near infrared interferometry, we intend to resolve the photosphere of RSGs and to bring new constraints on their modeling.
Methods. We observed the nearby RSG Antares using the four-telescope instrument VLTI/PIONIER. We collected data on the three available configurations of the 1.8m telescopes in the H band.
Results. We obtained unprecedented angular resolution on the disk of a star (6% of the star angular diameter) that limits the mean size of convective cells and offers new constraints on numerical simulations. Using an analytical model with a distribution of bright spots we determine their effect on the visibility signal.
Conclusions. We determine that the interferometric signal on Antares is compatible with convective cells of various sizes from 45% to 5% of the angular diameter. We also conclude that convective cells can strongly affect the angular diameter and limb-darkening measurements. In particular, the apparent angular diameter becomes dependent on the sampled position angles.

Abstract Copyright: © ESO, 2017

Journal keyword(s): stars: individual: Antares - stars: imaging - supergiants - stars: mass-loss - infrared: stars - techniques: interferometric - techniques: interferometric

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* V466 Cas s*r 01 19 53.6180547504 +58 18 30.745534716 13.04 10.74 8.62 6.86 5.44 M0.5Ib 79 0
2 V* T Per s*r 02 19 21.8771659920 +58 57 40.345527636 13.40 10.78 8.45 6.58 4.94 M2Iab 108 0
3 V* RS Per s*r 02 22 24.2955658080 +57 06 34.102933812 12.37 10.09 8.7680     M3.5IabFe-1 143 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 1670 0
5 HD 142407 * 15 55 30.5330032392 -31 05 01.019758020   7.581 6.199     K4III 18 0
6 HD 143787 PM* 16 03 20.6231448768 -25 51 54.873258444   6.202 4.966     K3III 46 0
7 HD 143900 * 16 03 54.7026524160 -24 43 34.728134052   7.621 6.211     K2/3III 23 0
8 * psi Oph PM* 16 24 06.1777460190 -20 02 14.352188619 6.37 5.53 4.50 3.72 3.22 K0-II-III 83 0
9 * alf Sco B Em* 16 29 24.20 -26 25 51.0   5.0 5.2     B2.5V 116 0
10 * 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 746 0
11 HD 148643 * 16 30 34.9685176272 -27 10 35.246558568   9.52 7.81     K3III 11 0
12 * phi Oph PM* 16 31 08.3669673955 -16 36 45.831122231 5.90 5.19 4.27 3.62 3.18 G8+IIIa 121 0
13 HD 148760 * 16 31 22.8479013264 -26 32 15.520616484   7.169 6.081     K1III 40 0
14 * alf Her ** 17 14 38.85818 +14 23 25.2262           M5Ib-II+G5III+F2V: 202 0

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