2017A&A...600A.136P


Query : 2017A&A...600A.136P

2017A&A...600A.136P - Astronomy and Astrophysics, volume 600A136-136 (2017/4-1)

The VLTI/MIDI view on the inner mass loss of evolved stars from the Herschel MESS sample.

PALADINI C., KLOTZ D., SACUTO S., LAGADEC E., WITTKOWSKI M., RICHICHI A., HRON J., JORISSEN A., GROENEWEGEN M.A.T., KERSCHBAUM F., VERHOELST T., RAU G., OLOFSSON H., ZHAO-GEISLER R. and MATTER A.

Abstract (from CDS):

Context. The mass-loss process from evolved stars is a key ingredient for our understanding of many fields of astrophysics, including stellar evolution and the chemical enrichment of the interstellar medium (ISM) via stellar yields. Nevertheless, many questions are still unsolved, one of which is the geometry of the mass-loss process.
Aims. Taking advantage of the results from the Herschel Mass loss of Evolved StarS (MESS) programme, we initiated a coordinated effort to characterise the geometry of mass loss from evolved red giants at various spatial scales.
Methods. For this purpose we used the MID-infrared interferometric Instrument (MIDI) to resolve the inner envelope of 14 asymptotic giant branch stars (AGBs) in the MESS sample. In this contribution we present an overview of the interferometric data collected within the frame of our Large Programme, and we also add archive data for completeness. We studied the geometry of the inner atmosphere by comparing the observations with predictions from different geometric models.
Results. Asymmetries are detected for the following five stars: R Leo, RT Vir, π1Gruis, omi Ori, and R Crt. All the objects are O-rich or S-type, suggesting that asymmetries in the N band are more common among stars with such chemistry. We speculate that this fact is related to the characteristics of the dust grains. Except for one star, no interferometric variability is detected, i.e. the changes in size of the shells of non-mira stars correspond to changes of the visibility of less than 10%. The observed spectral variability confirms previous findings from the literature. The detection of dust in our sample follows the location of the AGBs in the IRAS colour-colour diagram: more dust is detected around oxygen-rich stars in region II and in the carbon stars in region VII. The SiC dust feature does not appear in the visibility spectrum of the U Ant and S Sct, which are two carbon stars with detached shells. This finding has implications for the theory of SiC dust formation.

Abstract Copyright: © ESO, 2017

Journal keyword(s): stars: AGB and post-AGB - stars: mass-loss - circumstellar matter - techniques: high angular resolution - techniques: interferometric - techniques: interferometric

Simbad objects: 47

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Number of rows : 47
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 * 30 Psc LP? 00 01 57.6194717328 -06 00 50.654004048 7.88 6.04 4.41 2.85 1.44 M3III 152 0
2 * 7 Cet LP? 00 14 38.4169134264 -18 55 58.308074157 8.07 6.12 4.46 3.06 1.92 M1III 101 0
3 V* R For C* 02 29 15.3077617632 -26 05 55.646585700   12.94 7.50 8.01   C4,3e 206 0
4 * alf Cet LP? 03 02 16.77307 +04 05 23.0596 6.10 4.17 2.53 1.18 0.02 M1.5IIIa 480 1
5 * tau04 Eri LP* 03 19 31.0006476952 -21 45 28.315429163 7.13 5.32 3.70 2.12 0.66 M3III-IIIaCa-1 120 0
6 * gam Eri LP? 03 58 01.7658213057 -13 30 30.653301544 6.52 4.54 2.94 1.68 0.68 M0III-IIIb 200 0
7 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
8 * omi Ori S* 04 52 31.9624004856 +14 15 02.311506180   6.458 4.721     M3SIII 225 0
9 V* R Lep C* 04 59 36.3486921120 -14 48 22.502479140 15.06 13.51 7.76 4.90 3.42 C7,6e 360 0
10 * eps Lep PM* 05 05 27.6644072506 -22 22 15.724153311 6.41 4.64 3.18 2.08 1.27 K4III 169 0
11 * bet Col PM* 05 50 57.5922846925 -35 46 05.914636356 5.49 4.28 3.12 2.27 1.69 K1III_CN+1 153 0
12 * alf Car * 06 23 57.10988 -52 41 44.3810 -0.49 -0.59 -0.74 -0.96 -1.13 A9II 461 1
13 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A0mA1Va 1610 0
14 * 17 Mon * 06 47 19.8301708488 +08 02 14.122870224 7.82 6.17 4.77 3.74 3.04 K4III 125 0
15 * tet CMa PM* 06 54 11.3988612864 -12 02 19.061163780 7.20 5.51 4.08 2.95 2.17 K3/4III 233 0
16 V* BM Gem C* 07 20 59.0073521904 +24 59 58.086063708     11.50     C-J5- 155 1
17 * alf CMi SB* 07 39 18.11950 +05 13 29.9552 0.82 0.79 0.37 -0.05 -0.28 F5IV-V+DQZ 1925 0
18 * alf Hya * 09 27 35.24270 -08 39 30.9583 5.14 3.42 1.97 0.93 0.16 K3IIIa 455 1
19 V* R Leo Mi* 09 47 33.4839808805 +11 25 43.823283729 9.22 8.94 7.53 3.39 0.12 M7-9e 943 1
20 V* U Ant C* 10 35 12.8510147472 -39 33 45.324020448 15.32 8.22 5.38 3.18 1.86 C-N3 162 0
21 V* V Hya C* 10 51 37.2615873024 -21 15 00.333928044   12.23 6.80 7.42   C-N:6 391 0
22 V* R Crt AB* 11 00 33.8525664720 -18 19 29.582708520   10.33 9.80     M7/8III 222 0
23 * psi Vir LP* 12 54 21.1630369857 -09 32 20.360128902 7.94 6.39 4.80 3.23 1.95 M3-III 173 0
24 V* RT Vir AB* 13 02 37.9814644272 +05 11 08.362884984 10.07 9.07 7.41     M8III 336 0
25 * g Cen LP* 13 49 26.7219319935 -34 27 02.784711526 7.15 5.69 4.19 2.06 0.19 M5-III: 146 0
26 * tet Aps AB* 14 05 19.8809399288 -76 47 48.342695604 8.10 7.05 5.50     M6.5III: 127 0
27 * tet Cen PM* 14 06 40.94752 -36 22 11.8371 3.94 3.04 2.05 1.29 0.76 K0-IIIb 262 1
28 * c01 Cen PM* 14 43 39.4375747161 -35 10 25.206876063   5.41 4.04     K3IIIb 78 0
29 * sig Lib Mi* 15 04 04.2148093680 -25 16 55.090486596 6.86 4.91 3.21 1.60 0.33 M2.5III 195 0
30 V* X TrA C* 15 14 19.1755012584 -70 04 46.113298104 15.88 9.19 5.81     C5,5 130 0
31 V* V Oph C* 16 26 43.7067710136 -12 25 35.816948688   12.91 7.30     C-N:4 154 0
32 * alf TrA * 16 48 39.89508 -69 01 39.7626   3.33 1.88     K2III_Ba1 251 0
33 * eta Ara * 16 49 47.1562913570 -59 02 28.965649640   5.306 3.744     K5III 74 0
34 * zet Ara * 16 58 37.2125360584 -55 59 24.499906233   4.701 3.076     K3III 108 0
35 * gam02 Sgr PM* 18 05 48.4880988 -30 25 26.723458 4.77 4.00 2.99 2.26 1.75 K0+III 158 0
36 * eta Sgr LP? 18 17 37.6371989461 -36 45 42.084592381 6.37 4.67 3.11 1.55 0.23 M2III 149 0
37 * del Sgr * 18 20 59.6428936493 -29 49 41.168145329   4.069 2.668     K2.5IIIaCN0.5 184 0
38 * lam Sgr PM* 18 27 58.2407185 -25 25 18.114589 4.75 3.85 2.81 2.06 1.50 K1IIIb 290 0
39 V* S Sct C* 18 50 20.0367791256 -07 54 27.429169356 13.93 9.89 6.80     C-N5 215 0
40 * tau Sgr PM* 19 06 56.4031131168 -27 40 13.496293992 5.65 4.51 3.31 2.44 1.85 K1.5IIIb 164 0
41 V* AQ Sgr C* 19 34 18.9945475487 -16 22 27.048908541 13.85 9.48 6.70     C-N5 124 0
42 V* T Mic AB* 20 27 55.1897976672 -28 15 39.797839548   8.33 6.74     M7/8III 101 0
43 V* Y Pav C* 21 24 16.7499375384 -69 44 01.960245204 12.63 9.23 6.41     C7,3 89 0
44 * eps Peg LP* 21 44 11.1561394 +09 52 30.031152 5.61 3.91 2.39 1.34 0.58 K2Ib-II 464 1
45 * pi.01 Gru S* 22 22 44.2083897000 -45 56 52.791160956 10.52 8.62 6.55 3.19 0.52 S5,7: 216 0
46 * bet Gru LP? 22 42 40.05027 -46 53 04.4752 5.33 3.73 2.11 0.20 -1.57 M4.5III 209 1
47 * 19 Psc C* 23 46 23.5164473376 +03 29 12.519049272 10.95 7.62 5.02 3.19 1.82 C-N6 462 0

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