2024A&A...684A..77A


Query : 2024A&A...684A..77A

2024A&A...684A..77A - Astronomy and Astrophysics, volume 684A77 (2024/4-1)

CO emission survey of asymptotic giant branch stars with ultraviolet excesses.

ALONSO-HERNANDEZ J., SANCHEZ CONTRERAS C. and SAHAI R.

Abstract (from CDS):

Context. The transition from the spherically symmetric envelopes around asymptotic giant branch (AGB) stars to the asymmetric morphologies observed in planetary nebulae is still not well understood, and the shaping mechanisms are a subject of debate. Even though binarity is widely accepted as a promising option, it is limited by the complication of identifying binary AGB stars observationally. Recently, the presence of ultraviolet excesses in AGB stars has been suggested as a potential indicator of binarity.
Aims. Our main goals are to characterise the properties of the circumstellar envelopes (CSEs) around candidate AGB binary stars, specifically those selected based on their UV excess emission, and to compare these properties with those derived from previous CO-based studies of AGB stars.
Methods. We observed the 12CO (J=1-0) and 12CO (J=2-1) millimetre-wavelength emission in a sample of 29 AGB binary candidates with the IRAM-30 m antenna. We measured the systemic velocities and the terminal expansion velocities from their line profiles. Population diagrams were used to interpret the results, enabling the estimation of excitation temperatures (Tex), mass-loss rates (Ṁ), and the characteristic sizes of the envelope layers where the CO millimetre emission originates (Rs). We explored different trends between the envelope parameters deduced, multiwavelength flux measurements, and other properties of our sample, and compared them with those previously derived from larger samples of AGB stars found in the literature.
Results. We detected 12CO emission in 15 sources, of which 5 are first detections. We found relatively low expansion velocities (3 km s–1 ≲ Vexp ≲ 20 km s–1) in our sample. We derived the average excitation temperature and column density of the CO-emitting layers, which we used to estimate self-consistently the average mass-loss rate (10–8M⊙ yr–1 ≲ Ṁ ≲ 10–5M⊙ yr–1) and the CO pho-todissociation radius (5 × 1015 cm ≲ RCO ≲ 2 × 1017 cm) of our targets. We find a correlation between CO intensity and IRAS 60 µm fluxes, revealing a CO-to-IRAS 60 µm ratio lower than for AGB stars and closer to that found for pre-planetary nebulae (pPNe). An anti-correlation is observed between 12CO (and IRAS 60 µm) and the near-ultraviolet (NUV), but no such correlation is observed with the far-ultraviolet (FUV). It is also worth noting that there is no correlation between bolometric luminosity and NUV or FUV.
Conclusions. For the first time we have studied the mass-loss properties of UV-excess AGB binary candidates and estimated their main CSE parameters. Our sample of uvAGB stars shows similarities with the broader category of AGB stars, except for a distinct CO-to-IRAS 60 µm trend suggesting enhanced CO photodissociation. Our findings, based on single-dish low-J CO line emission observations, support the dust-driven wind scenario and indicate that alternative mass-loss mechanisms are not necessary (in principle) to explain the ∼200-2000 yr old mass-loss ejecta in uvAGBs. The different relationships between 12CO and IRAS 60 µm, with NUV and FUV are consistent with an intrinsic origin of NUV emission, but potential dominance of an extrinsic process (e.g. presence of a binary companion) in FUV emission.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: AGB and post-AGB - binaries: close - circumstellar matter - stars: mass-loss - radio lines: stars - ultraviolet: stars

Errata: erratum vol. 692, art. C4 (2024)

Simbad objects: 31

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Number of rows : 31
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 V* TU And Mi* 00 32 22.7282685288 +26 01 45.921110808   11.18 10.22 7.80   M6e 81 0
2 * omi Cet Mi* 02 19 20.79210 -02 58 39.4956   7.63 6.53 5.03   M5-9IIIe+DA 1586 0
3 V* RR Eri AB* 02 52 14.1850966152 -08 16 01.430627268   8.59 7.16     M5III 63 0
4 V* BD Cam Sy* 03 42 09.3255143544 +63 13 00.468590376 8.56 6.74 5.11 3.49 2.11 S3.5/2 220 0
5 V* V Eri AB* 04 04 18.8000912980 -15 43 30.499742695   10.405 9.146 8.912   M7+II: 92 0
6 V* Y Gem Sy* 07 41 08.5237339920 +20 25 44.334137208   10.23 9.09     M8 52 0
7 V* BC CMi LP* 07 52 07.1897763792 +03 16 38.436929508   7.85 6.39     M4/5III 50 0
8 V* RZ UMa AB* 08 10 59.7412493352 +65 13 22.121961384   10.84 9.63     M8 47 0
9 V* Z Cnc AB* 08 22 25.2910564920 +14 59 31.899972372   9.83 8.55     M6III 70 0
10 V* EY Hya Mi* 08 46 21.2058337320 +01 37 56.041768380   10.73 9.37     M7 52 0
11 V* RT Cnc AB* 08 58 15.9993994296 +10 50 42.676559520 10.04 8.97 7.52     M5III 63 1
12 V* IN Hya LP* 09 20 36.6822884904 +00 10 54.139721628   8.287 6.698     M3/4III 54 0
13 V* CG UMa LP* 09 21 43.2878012736 +56 41 57.193537416   7.08 5.47     M4IIIa 56 0
14 V* DF Leo LP* 09 23 29.5421486856 +07 42 49.494024864   8.48 6.89     M4III 34 0
15 V* R LMi OH* 09 45 34.2840467232 +34 30 42.809054724   9.442 8.443 9.024   M6.5-9e 343 0
16 IRC +10216 C* 09 47 57.40632 +13 16 43.5648           C9,5e 2455 0
17 V* UY Leo LP* 10 29 21.6231456936 +23 03 43.557694164   10.95 9.84     M7III: 26 0
18 V* R UMa Mi* 10 44 38.4723312408 +68 46 32.682649980   9.51 8.41     M5-8e 194 1
19 V* VY UMa C* 10 45 04.0305312384 +67 24 40.979062260 12.91 8.34 5.95 4.20 2.94 C-N5 209 0
20 V* ST UMa AB* 11 27 50.3780355120 +45 11 06.735697980 9.660 7.960 6.280     M4III 79 0
21 * ome Vir LP* 11 38 27.6074536027 +08 08 03.459408149 8.46 6.93 5.36     M4.5:III 121 0
22 V* FH Vir LP* 13 16 23.9303901120 +06 30 16.618728060   8.63 7.21     M6III 49 0
23 V* BY Boo LP? 14 07 55.7554099635 +43 51 16.028575533 8.52 6.86 5.28 3.43 1.77 M4.5III 186 0
24 V* RW Boo AB* 14 41 13.3762067784 +31 34 19.711947072 10.23 9.34 8.00     M5III: 70 0
25 V* RR UMi LP* 14 57 35.0095879431 +65 55 56.814643584 7.86 6.19 4.54 2.69 0.97 M4.5III 195 0
26 V* Y CrB AB* 15 46 43.7151616656 +38 19 20.561578428   11.62 10.45     M8III: 33 0
27 V* RU Her Mi* 16 10 14.5126789272 +25 04 14.306977524   13.82 12.24 7.56 4.15 M6-7e 224 0
28 V* AT Dra LP* 16 17 15.3511289064 +59 45 18.060635412 8.70 7.03 5.40     M4III 68 0
29 V* T Dra C* 17 56 23.3288487384 +58 13 06.783372804   18.08 7.20 9.39   C6,2e 203 0
30 V* SV Peg AB* 22 05 42.0835861728 +35 20 54.562625016   10.06 9.20     M7 146 0
31 V* W Peg Mi* 23 19 50.5014315096 +26 16 43.665640932   10.69 7.60 6.45   M6.5-7.5e 126 0

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