2021A&A...653A..53A


Query : 2021A&A...653A..53A

2021A&A...653A..53A - Astronomy and Astrophysics, volume 653A53-53 (2021/9-1)

DEATHSTAR: nearby AGB stars with the Atacama Compact Array. II. CO envelope sizes and asymmetries: the S-type stars.

ANDRIANTSARALAZA M., RAMSTEDT S., VLEMMINGS W.H.T., DANILOVICH T., DE BECK E., GROENEWEGEN M.A.T., HOFNER S., KERSCHBAUM F., KHOURI T., LINDQVIST M., MAERCKER M., OLOFSSON H., QUINTANA-LACACI G., SABERI M., SAHAI R. and ZIJLSTRA A.

Abstract (from CDS):


Aims. We aim to constrain the sizes of, and investigate deviations from spherical symmetry in, the CO circumstellar envelopes (CSEs) of 16 S-type stars, along with an additional 7 and 4 CSEs of C-type and M-type AGB stars, respectively.
Methods. We map the emission from the CO J=2-1 and 3-2 lines observed with the Atacama Compact Array (ACA) and its total power (TP) antennas, and fit with a Gaussian distribution in the uv- and image planes for ACA-only and TP observations, respectively. The major axis of the fitted Gaussian for the CO(2-1) line data gives a first estimate of the size of the CO-line-emitting CSE. We investigate possible signs of deviation from spherical symmetry by analysing the line profiles and the minor-to-major axis ratio obtained from visibility fitting, and by investigating the deconvolved images.
Results. The sizes of the CO-line-emitting CSEs of low-mass-loss-rate (low-MLR) S-type stars fall between the sizes of the CSEs of C-stars, which are larger, and those of M-stars, which are smaller, as expected because of the differences in their respective CO abundances and the dependence of the photodissociation rate on this quantity. The sizes of the low-MLR S-type stars show no dependence on circumstellar density, as measured by the ratio of the MLR to terminal outflow velocity, irrespective of variability type. The density dependence steepens for S-stars with higher MLRs. While the CO(2-1) brightness distribution size of the low-density S-stars is in general smaller than the predicted photodissociation radius (assuming the standard interstellar radiation field), the measured size of a few of the high-density sources is of the same order as the expected photodissociation radius. Furthermore, our results show that the CO CSEs of most of the S-stars in our sample are consistent with a spherically symmetric and smooth outflow. For some of the sources, clear and prominent asymmetric features are observed which are indicative of intrinsic circumstellar anisotropy.
Conclusions. As the majority of the S-type CSEs of the stars in our sample are consistent with a spherical geometry, the CO envelope sizes obtained in this paper will be used to constrain detailed radiative transfer modelling to directly determine more accurate MLR estimates for the stars in our sample. For several of our sources that present signs of deviation from spherical symmetry, further high-resolution observations would be necessary to investigate the nature of, and the physical processes behind, these asymmetrical structures. This will provide further insight into the mass-loss process and its related chemistry in S-type AGB stars.

Abstract Copyright: © ESO 2021

Journal keyword(s): stars: AGB and post-AGB - stars: mass-loss - stars: winds, outflows - circumstellar matter

VizieR on-line data: <Available at CDS (J/A+A/653/A53): stars.dat list.dat fits/*>

Simbad objects: 29

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Number of rows : 29
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 BD-15 6542 * 00 05 54.8414783400 -14 25 58.058430420   10.091 9.663     G0 15 0
2 V* T Cet S* 00 21 46.2726376677 -20 03 28.888739999   7.32 5.74     M5-6Se 156 0
3 V* U Men OH* 04 09 35.5833357218 -81 51 17.682061033           M3e 65 0
4 V* R Dor AB* 04 36 45.59127 -62 04 37.7974 7.84 6.98 5.40 2.71 -0.44 M8III:e 376 0
5 V* FU Mon S* 06 22 23.8515787464 +03 25 27.887405916 16.86 12.36 9.06     S6.5/7.5 124 1
6 V* DY Gem S* 06 35 57.8113561320 +14 12 46.026222696   11.40 11.20     S8,5 62 0
7 RAFGL 4078 C* 07 45 02.4149777160 -71 19 45.862198392       15.92 12.72 C 64 0
8 V* Z Ant S* 10 45 58.8770905272 -35 15 04.401660600   11.38 10.00     S5,4 34 0
9 V* UY Cen S* 13 16 31.8299380416 -44 42 15.757651800 14.09 10.03 7.13     S6/8 91 0
10 V* TT Cen S* 13 19 35.0158771776 -60 46 46.295369400     11.50     SC5:/8+ 60 0
11 V* AM Cen S* 13 47 17.6163269400 -53 21 25.926046632   11.50 9.20 8.40   SC 44 0
12 V* V1302 Cen C* 13 58 17.1148962816 -56 21 11.298686220   10.43 7.44     C 37 0
13 * tet Aps AB* 14 05 19.8809399288 -76 47 48.342695604 8.10 7.05 5.50     M6.5III: 127 0
14 V* V996 Cen C* 14 14 07.3492293528 -53 55 55.167963528   10.55 7.25     C 44 0
15 V* GI Lup S* 15 06 16.3144281432 -41 28 13.869517044     10.40     S7,8e 40 0
16 V* X TrA C* 15 14 19.1755012584 -70 04 46.113298104 15.88 9.19 5.81     C5,5 130 0
17 V* ST Sco S* 16 36 36.2192115984 -31 14 02.427110736   11.36 10.40     S8/4.5 55 0
18 V* RT Sco S* 17 03 32.5593710616 -36 55 13.694502792       13.973   S7,2 76 0
19 IRC -10401 S* 18 10 24.8131426752 -10 34 15.909217320     16     M7S 32 0
20 IRC +20370 C* 18 41 54.5501446200 +17 41 08.425834728       13.56   C7,3e 124 0
21 IRC -30398 Mi* 18 59 13.8469390704 -29 50 20.513684796   14.35 14.19 15.46   M9 49 0
22 V* ST Sgr S* 19 01 29.1966290472 -12 45 34.097956812   12.13 7.20     S6-7.5/2.5e 80 0
23 V* W Aql S* 19 15 23.3572741560 -07 02 50.333886492   12.72 10.14 10.21   S6/6e 251 0
24 V* T Sgr S* 19 16 14.4361485576 -16 58 17.076889992   11.81 7.10     S4.5-6/5.5-6e 143 0
25 V* AQ Sgr C* 19 34 18.9945475487 -16 22 27.048908541 13.85 9.48 6.70     C-N5 124 0
26 RAFGL 2425 OH* 19 39 00.7388220744 -16 51 56.630561580           M10III 58 0
27 V* RZ Sgr S* 20 15 28.4023889376 -44 24 37.478466072   10.550 9.533 7.858   S4,4ep 79 0
28 * 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
29 RAFGL 3068 C* 23 19 12.60744 +17 11 33.1332           C 288 1

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