2022A&A...660A..94G


Query : 2022A&A...660A..94G

2022A&A...660A..94G - Astronomy and Astrophysics, volume 660A94-94 (2022/4-1)

ATOMIUM: ALMA tracing the origins of molecules in dust forming oxygen rich M-type stars. Motivation, sample, calibration, and initial results.

GOTTLIEB C.A., DECIN L., RICHARDS A.M.S., DE CEUSTER F., HOMAN W., WALLSTROM S.H.J., DANILOVICH T., MILLAR T.J., MONTARGES M., WONG K.T., McDONALD I., BAUDRY A., BOLTE J., CANNON E., DE BECK E., DE KOTER A., EL MELLAH I., ETOKA S., GOBRECHT D., GRAY M., HERPIN F., JESTE M., KERVELLA P., KHOURI T., LAGADEC E., MAES S., MALFAIT J., MENTEN K.M., MULLER H.S.P., PIMPANUWAT B., PLANE J.M.C., SAHAI R., VAN DE SANDE M., WATERS L.B.F.M., YATES J. and ZIJLSTRA A.

Abstract (from CDS):

This overview paper presents ATOMIUM, a Large Programme in Cycle 6 with the Atacama Large Millimeter/submillimeter Array (ALMA). The goal of ATOMIUM is to understand the dynamics and the gas phase and dust formation chemistry in the winds of evolved asymptotic giant branch (AGB) and red supergiant (RSG) stars. A more general aim is to identify chemical processes applicable to other astrophysical environments. Seventeen oxygen-rich AGB and RSG stars spanning a range in (circum)stellar parameters and evolutionary phases were observed in a homogeneous observing strategy allowing for an unambiguous comparison. Data were obtained between 213.83 and 269.71 GHz at high (∼0.025''-0.050''), medium (∼0.13''-0.24''), and low (∼1'') angular resolution. The sensitivity per ∼1.3 km s–1 channel was 1.5-5 mJy beam–1, and the line-free channels were used to image the millimetre wave continuum. Our primary molecules for studying the gas dynamics and dust formation are CO, SiO, AlO, AlOH, TiO, TiO2, and HCN; secondary molecules include SO, SO2, SiS, CS, H2O, and NaCl. The scientific motivation, survey design, sample properties, data reduction, and an overview of the data products are described. In addition, we highlight one scientific result - the wind kinematics of the ATOMIUM sources. Our analysis suggests that the ATOMIUM sources often have a slow wind acceleration, and a fraction of the gas reaches a velocity which can be up to a factor of two times larger than previously reported terminal velocities assuming isotropic expansion. Moreover, the wind kinematic profiles establish that the radial velocity described by the momentum equation for a spherical wind structure cannot capture the complexity of the velocity field. In fifteen sources, some molecular transitions other than 12CO v = 0 J = 2 - 1 reach a higher outflow velocity, with a spatial emission zone that is often greater than 30 stellar radii, but much less than the extent of CO. We propose that a binary interaction with a (sub)stellar companion may (partly) explain the non-monotonic behaviour of the projected velocity field. The ATOMIUM data hence provide a crucial benchmark for the wind dynamics of evolved stars in single and binary star models.

Abstract Copyright: © ESO 2022

Journal keyword(s): stars: AGB and post-AGB - stars: mass-loss - circumstellar matter - binaries: general - instrumentation: interferometers - astrochemistry

VizieR on-line data: <Available at CDS (J/A+A/660/A94): tablee1.dat>

Simbad objects: 52

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Number of rows : 52
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 3HSP J010326.0+152624 BLL 01 03 26.0003786544 +15 26 24.650787336   19.75 18.55 16.4   ~ 46 1
2 IRC +10011 OH* 01 06 25.9879717848 +12 35 52.896392052   20.7   18.26 14.01 M8 436 0
3 ICRF J011725.2+141812 Bla 01 17 25.20308969 +14 18 12.4203209       20.23   ~ 38 1
4 V* IK Tau OH* 03 53 28.8924743304 +11 24 21.895183368 16.99 14.463 16.171 14.101   M7-11 675 0
5 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
6 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
7 NAME Puppis reg 07 40 -28.0           ~ 108 0
8 IRC +10216 C* 09 47 57.40632 +13 16 43.5648           C9,5e 2455 0
9 QSO J1246-2547 Bla 12 46 46.80203943 -25 47 49.2889822   17.65 17.41 16.96 15.5 ~ 314 1
10 V* R Hya Mi* 13 29 42.7801586466 -23 16 52.751628992 7.26 6.58 4.97 2.27 -0.15 M6-9e 511 0
11 [VV2006] J133901.8-240114 BLL 13 39 01.74639481 -24 01 14.0062115   19.0 17.56 17.21   ~ 75 1
12 NGC 6061 Sy2 16 06 16.0278 +18 14 59.835   15.0 15.0     ~ 105 1
13 QSO J1619+2247 Bla 16 19 14.82460190 +22 47 47.8509104       20.00   ~ 77 1
14 V* U Her OH* 16 25 47.4719383584 +18 53 32.863368084 8.85 8.23 6.70     M6.5-8+e 563 1
15 V* AH Sco s*r 17 11 17.0194487616 -32 19 30.714035556   10.03 8.10     M5Ia-Iab 145 0
16 V* RW Sco OH* 17 14 51.6789006720 -33 25 54.539038236     11.06 10.07 8.71 M6e 80 0
17 ICRF J171736.0-334208 BLL 17 17 36.02929270 -33 42 08.8296186   20.93   17.3   ~ 136 1
18 QSO J1744-3116 Bla 17 44 23.57824 -31 16 36.2943           ~ 168 1
19 V* KW Sgr s*r 17 52 00.7269495408 -28 01 20.555654448   11.45 11.00     M3Ia 94 0
20 NVSS J175233-295645 Rad 17 52 33.10799805 -29 56 44.9191885           ~ 26 1
21 PMN J1755-2232 Rad 17 55 26.284538 -22 32 10.61562           ~ 38 1
22 V* VX Sgr s*r 18 08 04.0442790744 -22 13 26.600899044 11.72 9.41 6.52 3.90 2.11 M8.5Ia 622 0
23 ICRF J182912.4-581355 Bla 18 29 12.40235306 -58 13 55.1618061   19.26   18.80   ~ 50 1
24 NVSS J183211-203947 BLL 18 32 11.0455806144 -20 39 48.210054948   18.56 20.2     ~ 75 1
25 NVSS J190539+095208 Rad 19 05 39.89897022 +09 52 08.4074677           ~ 24 1
26 V* R Aql OH* 19 06 22.2510922392 +08 13 48.012661776 8.06 7.69 6.09     M6.5-9e 579 2
27 ICRF J190711.9+012708 QSO 19 07 11.99616361 +01 27 08.9617282           ~ 49 1
28 ICRF J191207.1-080421 QSO 19 12 07.12880916 -08 04 21.9024580           ~ 22 1
29 V* W Aql S* 19 15 23.3572741560 -07 02 50.333886492   12.72 10.14 10.21   S6/6e 251 0
30 NGC 6812 Bla 19 45 24.22882927 -55 20 48.8362978   13.58   11.91   ~ 63 1
31 PMN J1946-5812 rG 19 46 29.82760 -58 12 52.4163           ~ 7 1
32 V* GY Aql Mi* 19 50 06.3301987896 -07 36 52.465065516   12.54 11.22     M8 127 0
33 ICRF J195147.4-050943 Bla 19 51 47.46846027 -05 09 43.9624421       19.50   ~ 34 1
34 V* S Pav Mi* 19 55 13.9680387696 -59 11 44.333160288   9.25 8.21     M8III 95 0
35 IRC -10529 OH* 20 10 27.8731455576 -06 16 13.758742596         15.49 M: 153 0
36 ICRF J201857.7-050929 Bla 20 18 57.75991477 -05 09 29.3733350       18.96   ~ 28 1
37 QSO B2021-330 Bla 20 24 35.57645053 -32 53 35.9124670   18.73 16.3 18.70   ~ 79 1
38 QSO B2022-077 BLL 20 25 40.6602562440 -07 35 52.688047128   18.5       ~ 234 3
39 ICRF J202553.6-284548 QSO 20 25 53.61284023 -28 45 48.6983395       17.70   ~ 60 1
40 V* T Mic AB* 20 27 55.1897976672 -28 15 39.797839548   8.33 6.74     M7/8III 101 0
41 V* U Del AB* 20 45 28.2357324504 +18 05 24.138355308 9.30 8.06 6.38     M4-6II-III 134 0
42 ICRF J205135.5+174336 BLL 20 51 35.58294533 +17 43 36.9001514     18.0 14.41   ~ 41 1
43 QSO B2052-474 Bla 20 56 16.35980507 -47 14 47.6277179   18.29 19.1 18.07   ~ 341 1
44 ICRF J205625.0-320847 BLL 20 56 25.07022954 -32 08 47.8002638   20.5   17.60   ~ 34 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 QSO B2227-445 Bla 22 30 56.4428528280 -44 16 29.891303688     18.1 19.4   ~ 54 1
47 QSO B2245-328 Bla 22 48 38.68573790 -32 35 52.1881477   18.38 18.6 18.63   ~ 132 1
48 V* V PsA AB* 22 55 19.6832667720 -29 36 44.521985340   10.18 9.30     M7/8III 57 0
49 QSO B2255-2814 Bla 22 58 05.96287687 -27 58 21.2567572   17.34 16.77 17.20   ~ 397 1
50 V* SV Aqr AB* 23 22 45.3630843744 -10 49 00.064750908   10.91 9.83     M8 39 0
51 ICRF J232339.1-061759 QSO 23 23 39.11376282 -06 17 59.2393982           ~ 25 1
52 QSO J2345-1555 BLL 23 45 12.4622049264 -15 55 07.836801888   19.21   18.48   ~ 202 1

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