2017A&A...606A..20P


Query : 2017A&A...606A..20P

2017A&A...606A..20P - Astronomy and Astrophysics, volume 606A, 20-20 (2017/10-1)

Rubidium and zirconium abundances in massive Galactic asymptotic giant branch stars revisited.

PEREZ-MESA V., ZAMORA O., GARCIA-HERNANDEZ D.A., PLEZ B., MANCHADO A., KARAKAS A.I. and LUGARO M.

Abstract (from CDS):

Context. Luminous Galactic OH/IR stars have been identified as massive (>4-5M) asymptotic giant branch (AGB) stars experiencing hot bottom burning and Li production. Their Rb abundances and [Rb/Zr] ratios, as derived from classical hydrostatic model atmospheres, are significantly higher than predictions from AGB nucleosynthesis models, posing a problem for our understanding of AGB evolution and nucleosynthesis.
Aims. We report new Rb and Zr abundances in the full sample (21) of massive Galactic AGB stars, previously studied with hydrostatic models, by using more realistic extended model atmospheres.
Methods. For this, we use a modified version of the spectral synthesis code Turbospectrum and consider the presence of a circumstellar envelope and radial wind in the modelling of the optical spectra of these massive AGB stars. The Rb and Zr abundances are determined from the 7800Å Rb I resonant line and the 6474Å ZrO bandhead, respectively, and we explore the sensitivity of the derived abundances to variations of the stellar (Teff) and wind (M, β and vexp) parameters in the pseudo-dynamical models. The Rb and Zr abundances derived from the best spectral fits are compared with the most recent AGB nucleosynthesis theoretical predictions.
Results. The Rb abundances derived with the pseudo-dynamical models are much lower (in the most extreme stars even by ∼1-2 dex) than those derived with the hydrostatic models, while the Zr abundances are similar. The Rb I line profile and Rb abundance are very sensitive to the wind mass-loss rate M (especially for M≳10–8M/yr) but much less sensitive to variations of the wind velocity-law (β parameter) and the expansion velocity vexp(OH).
Conclusions. We confirm the earlier preliminary results based on a smaller sample of massive O-rich AGB stars, suggesting that the use of extended atmosphere models can solve the discrepancy between the AGB nucleosynthesis theoretical models and the observations of Galactic massive AGB stars. The Rb abundances, however, are still strongly dependent on the wind mass-loss M, which, unfortunately, is unknown in these AGB stars. Accurate mass-loss rates M (e.g. from rotationally excited lines of the CO isotopologues in the radio domain) in these massive Galactic AGB stars are needed in order to break the model's degeneracy and obtain reliable (non-model-dependent) Rb abundances in these stars.

Abstract Copyright: © ESO, 2017

Journal keyword(s): stars: AGB and post-AGB - stars: atmospheres - stars: abundances - stars: evolution - stars: late-type - nuclear reactions, nucleosynthesis, abundances - nuclear reactions, nucleosynthesis, abundances

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 - 2024
#notes
1 IC 1613 GiC 01 04 48.4071 +02 07 10.185   10.42 10.01 9.77   ~ 1236 2
2 IRC +10011 OH* 01 06 25.9879717848 +12 35 52.896392052   20.7   18.26 14.01 M8 420 0
3 IRC +30021 OH* 01 11 15.9306739944 +30 38 06.270834804       13.73   M10 80 1
4 OH 127.8-00.0 OH* 01 33 51.21048 +62 26 53.2032           O-rich 181 0
5 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7078 0
6 V* SY Men OH* 04 39 16.0791799392 -74 21 41.907210192           M9 30 0
7 V* T Lep Mi* 05 04 50.8451254800 -21 54 16.520551560   10.99 7.40     M6ev 148 0
8 V* U Dor OH* 05 10 08.8413498888 -64 19 04.255801500   11.86 8.10     M8IIIe 62 0
9 IRC +50137 OH* 05 11 19.4506093584 +52 52 33.235824324           M10 174 0
10 IRC +60154 OH* 05 19 52.1469619752 +63 15 54.963480240       16.24   M9 67 0
11 V* AP Lyn Mi* 06 34 33.3992529912 +60 56 27.812508252   12.51 11.15 11.90   M7+ 116 0
12 IRAS 07222-2005 Mi* 07 24 24.4245337224 -20 11 56.095515528     17.954   12.26 M9: 12 0
13 V* MQ Vel OH* 09 21 18.4676569224 -45 30 56.817261324           M7/9S? 12 0
14 V* VZ Vel OH* 10 28 11.0083798248 -51 11 07.684927008   11.96 10.87     M6e 23 0
15 IRAS 14266-4211 OH* 14 29 51.6394420440 -42 25 06.429698184           O-rich 8 0
16 V* S CrB Mi* 15 21 23.9553294936 +31 22 02.584877304 7.51 7.15 5.80 8.12   M6.5-8e 351 0
17 V* FS Lib OH* 16 00 23.7681792792 -12 20 57.331224456       13.802   M7/9 57 0
18 V* V1012 Her OH* 16 05 28.8972111504 +42 10 29.489337876           M8 24 0
19 V* V345 Nor Mi* 16 06 51.6849774312 -52 04 34.814139564     14.10     O-rich 12 1
20 V* V850 Oph Mi* 17 06 10.8048482688 -10 28 59.170261224     15     M8 24 0
21 OH 026.5+00.6 OH* 18 37 32.50920 -05 23 59.1936           O-rich 301 1
22 V* V3952 Sgr OH* 18 45 51.3278270352 -17 17 59.660446020   12.77 11.61     M9 28 0
23 IRC -20540 OH* 19 08 54.9247580040 -22 14 18.600288180     17 14.58 10.55 M8: 77 0
24 OH 044.8-02.3 OH* 19 21 36.6364189224 +09 27 56.688388992           O-rich 88 0
25 IRAS 19426+4342 OH* 19 44 15.9491719544 +43 49 19.515922016           O-rich 7 0
26 IRC +10451 OH* 20 07 43.0503248640 +06 03 11.971572300           M9 39 0
27 IRC -10529 OH* 20 10 27.8731455576 -06 16 13.758742596         15.49 M: 141 0
28 V* RT Mic Mi* 20 37 22.9200861336 -30 10 26.175840204           O-rich 20 0
29 RAFGL 2885 OH* 22 19 27.47784 +59 51 21.7080           O-rich 136 0

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