2022MNRAS.510...82R


Query : 2022MNRAS.510...82R

2022MNRAS.510...82R - Mon. Not. R. Astron. Soc., 510, 82-94 (2022/February-2)

Improving the diameters of interferometric calibrators with MATISSE.

ROBBE-DUBOIS S., CRUZALEBES P., BERIO P., MEILLAND A., PETROV R.-G., ALLOUCHE F., SALABERT D., PALADINI C., MATTER A., MILLOUR F., LAGARDE S., LOPEZ B., BURTSCHER L., JAFFE W., HRON J., PERCHERON I., VAN BOEKEL R., WEIGELT G. and STEE P.

Abstract (from CDS):

A good knowledge of the angular diameters of stars used to calibrate the observables in stellar interferometry is fundamental. As the available precision for giant stars is worse than the required per cent level, we aim to improve the knowledge of many diameters using MATISSE (Multiple AperTure mid-Infrared SpectroScopic Experiment) data in its different instrumental configurations. Using the squared visibility MATISSE observable, we compute the angular diameter value, which ensures the best-fitting curves, assuming an intensity distribution of a uniform disc. We take into account that the transfer function varies over the wavelength and is different from one instrumental configuration to another. The uncertainties on the diameters are estimated using the residual bootstrap method. Using the low spectral resolution mode in the Lband, we observed a set of 35 potential calibrators selected in the Mid-infrared stellar Diameter and Flux Compilation Catalogue with diameters ranging from about 1 to 3 mas. We reach a precision on the diameter estimates in the range 0.6 per cent to 4.1 per cent. The study of the stability of the transfer function in visibility over two nights makes us confident in our results. In addition, we identify one star, 75 Vir initially present in the calibrator lists, for which our method does not converge, and prove to be a binary star. This leads us to the conclusion that our method is actually necessary to improve the quality of the astrophysical results obtained with MATISSE, and that it can be used as a useful tool for 'bad calibrator' detection.

Abstract Copyright: © 2021 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): methods: numerical - methods: observational - techniques: high angular resolution - techniques: interferometric - infrared: stars

Simbad objects: 40

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Number of rows : 40
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 * 7 Cet LP? 00 14 38.4169134264 -18 55 58.308074157 8.07 6.12 4.46 3.06 1.92 M1III 101 0
2 HD 1089 PM* 00 14 58.2617231904 -34 54 15.202152108   7.526 6.159     K3III 20 0
3 HD 1923 V* 00 23 22.1450884920 -29 50 50.109150264 10.21 8.38 6.82     M2III 28 0
4 HD 3605 PM* 00 38 48.7830987696 -25 06 28.140485904   7.90 6.41     K4III 18 0
5 V* R Scl C* 01 26 58.0939182720 -32 32 35.439234828 17.26 9.59 5.72 3.69 2.30 C-N5+ 354 0
6 * mu. Psc PM* 01 30 11.1150260499 +06 08 37.758162354 7.75 6.22 4.84 3.78 3.04 K3III 192 0
7 * nu. Psc * 01 41 25.8941428289 +05 29 15.401884416 7.36 5.81 4.44 3.38 2.67 K3III 248 0
8 * chi Eri PM* 01 55 57.4597664541 -51 36 31.959325912   4.55 3.71     G8IIIbCNIV 149 0
9 HD 15652 * 02 30 32.7936318696 -22 32 43.146094452   7.722 6.148     M0III 33 0
10 * nu. Cet SB* 02 35 52.4740495740 +05 35 35.664001770   5.742 4.871     G8III 97 0
11 HD 17973 No* 02 53 38.4814287600 +14 40 12.916420212   8.4 7.56 6.7   ~ 19 0
12 HD 19723 * 03 10 49.1572717440 +10 00 21.239863596   8.68 6.97     K2 13 0
13 HD 20356 * 03 16 21.7233171936 -05 43 49.673021736   7.92 6.31     K4III 25 0
14 * pi. Eri LP? 03 46 08.5352200200 -12 06 05.718535236 8.05 6.04 4.42 3.08 2.03 M1III 64 0
15 * eps Lep PM* 05 05 27.6644072506 -22 22 15.724153311 6.41 4.64 3.18 2.08 1.27 K4III 169 0
16 HD 45677 Be* 06 28 17.4219710352 -13 03 11.128860972 7.86 8.52 8.50 8.11 8.01 B2IV/V[e] 343 0
17 * 28 Hya * 09 25 24.0350848224 -05 07 02.622641052   7.082 5.579     K4/5III 53 0
18 * 18 Leo * 09 46 23.3273119968 +11 48 36.155648304   7.142 5.644     K4III 58 0
19 * 26 Sex * 10 26 36.9146017200 -00 59 17.002863096   7.773 6.305     K3III 20 0
20 HD 90798 V* 10 28 02.0952416304 -49 24 20.888342172   7.583 6.086     K4III 21 0
21 HD 94014 PM* 10 51 05.4081454560 -03 05 33.600197652   7.427 5.941     K4/5III 19 0
22 * iot Ant PM* 10 56 43.0512189504 -37 08 15.962675568 6.47 5.63 4.60 3.85 3.32 K0III 58 0
23 * 35 Vir AB* 12 47 51.4128281376 +03 34 21.770544288 9.84 8.01 6.41     M0/1III 42 0
24 * 75 Vir PM* 13 32 51.6427709058 -15 21 46.848592268   6.760 5.529     K1.5IIIb: 25 0
25 * 106 Vir PM* 14 28 41.7223108944 -06 54 01.897156080   6.901 5.418     K4/5III 37 0
26 * nu. Lib * 15 06 37.5965113128 -16 15 24.546990276 8.70 6.78 5.20     K5-III 100 0
27 HD 135367 * 15 14 50.5965397992 -05 30 09.186893460   7.80 6.29     K3III 18 0
28 * 37 Lib PM* 15 34 10.7024841438 -10 03 52.317750492 6.48 5.63 4.62 3.85 3.33 K1III-IV 187 0
29 HD 138938 * 15 36 12.9057527928 -28 59 55.866989760   8.57 6.92     K5III 6 0
30 HD 145085 * 16 08 58.8793121880 +03 27 16.108892424   7.406 5.909     K4III 35 0
31 HD 153113 * 16 57 20.2491354912 +06 12 40.692542832   8.25 6.72     K0 13 0
32 V* V849 Ara s*r 17 00 55.6979177040 -56 28 48.030444372   9.92 8.28     M3/4Ib 20 0
33 HD 162774 V* 17 52 35.4392568576 +01 18 18.039891744   7.479 5.917     K4III 25 0
34 * eta Ser PM* 18 21 18.6004923875 -02 53 55.780691633 4.84 4.19 3.25 2.55 2.05 K0III-IV 390 0
35 * e01 Sgr PM* 19 40 43.3830302448 -16 17 35.774383560   6.415 5.296     K1III 88 0
36 HD 184996 PM* 19 41 37.2651271392 -65 51 15.890900436   7.639 6.074     M0III 23 0
37 HD 186251 PM* 19 47 05.8141738776 -62 27 13.344343092   8.30 6.70     M2III 15 0
38 HD 189695 * 20 00 58.9762436208 +08 33 27.850936644 9.32 7.43 5.91     K5III 35 0
39 V* LU Aqr LP* 23 28 07.2657598056 -12 12 44.372899944   8.91 7.53     K3III 13 0
40 * 104 Aqr * 23 41 45.8063762520 -17 48 59.515007076 6.14 5.65 4.83 4.22 3.80 G2Ib/II 111 0

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