2012A&A...538A..48P


Query : 2012A&A...538A..48P

2012A&A...538A..48P - Astronomy and Astrophysics, volume 538A48-48 (2012/2-1)

High-resolution spectroscopic observations of two s-process-enriched and carbon-poor post-AGB stars: GLMP 334 and IRAS 15482-5741.

PEREIRA C.B., GALLINO R. and BISTERZO S.

Abstract (from CDS):

The study of post-AGB stars provides important information on the s-process inside asymptotic giant branch (AGB) stars. We determined the atmospheric parameters and abundance patterns of two post-AGB stars: GLMP 334 and IRAS 15482-5741 to better understand their evolutionary state and the nature of the s-element enhancement of these stars. We used high-resolution optical spectroscopy. Atmospheric parameters and abundances were determined in the local-thermodynamic-equilibrium model atmospheres of Kurucz (1993, CD-ROM 13, SAO) using the spectral analysis code MOOG. Spectroscopic observations are compared with nucleosynthesis AGB models of different initial masses and s-process efficiencies. Theoretical interpretations are presented and discussed. The observed distribution of neutron capture elements can be fitted with particular choices of AGB initial masses and of the 13C neutron source (13C-pocket strengths) obtained at the adopted [Fe/H] for each star, but the low [C/Fe] observed is incompatible with model predictions. The problem can be solved by increasing the metallicity by 0.2dex, which is inside the spectroscopic uncertainty. The abundances of carbon and nitrogen observed in these stars may support the occurrence of an extra-mixing episode, the ``cool bottom process'', even if its exact effect cannot be theoretically quantified yet.

Abstract Copyright: ∼

Journal keyword(s): stars: AGB and post-AGB - stars: evolution - stars: abundances - stars: chemically peculiar

Simbad objects: 19

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Number of rows : 19
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 IRAS Z02229+6208 pA* 02 26 41.7882689568 +62 21 21.981286008   14.69 12.00 11.16 8.92 G8-K0_0-Ia: 65 0
2 IRAS 04296+3429 pA* 04 32 56.9743899192 +34 36 12.459816288   16.13 14.09 13.64 11.64 G0Ia 149 0
3 IRAS 05113+1347 pA* 05 14 07.7664787608 +13 50 28.200887160   14.786 12.574 11.663 10.26 G5I 72 0
4 IRAS 05341+0852 pA* 05 36 55.0511076432 +08 54 08.656315452   15.37 13.45 12.95 11.43 F5I 126 0
5 IRAS 06530-0213 pA* 06 55 31.8205478808 -02 17 28.243142520   16.38 13.99 13.26   F5Ia 87 0
6 HD 56126 pA* 07 16 10.2590823192 +09 59 47.954735376   9.20 8.32     F0/5Ia 330 0
7 IRAS 07430+1115 s*r 07 45 51.3968191368 +11 08 19.561606620   13.94 12.22 11.82 10.69 M2I 64 0
8 IRAS 08143-4406 pA* 08 16 03.0217187040 -44 16 04.640255580           F8I 33 0
9 IRAS 08281-4850 pA* 08 29 40.5522281112 -49 00 04.329698184       13.50   F0I 22 0
10 HD 89353 pA* 10 18 07.5899342712 -28 59 31.195183524   5.76 5.53     B9.5Ib/II 315 0
11 IRAS 12360-5740 pA* 12 38 53.1155012016 -57 56 31.843075416   13.541 12.399 12.128   ~ 19 0
12 IRAS 14325-6428 pA* 14 36 34.3740180048 -64 41 31.082196876   12.56 12.00     F5I 28 0
13 IRAS 15482-5741 pA? 15 52 19.4524895606 -57 50 53.200683691           ~ 16 0
14 HD 172481 pA* 18 41 36.9595215744 -27 57 01.235714652   9.58 9.06     F2/3Ia 52 0
15 IRAS 19386+0155 pA* 19 41 08.2923311712 +02 02 31.208770140   12.32 11.20     F5Ib 44 0
16 HD 187885 pA* 19 52 52.7033593752 -17 01 50.289441096   9.25 8.68 8.32   F2/6Ia 185 0
17 V* V448 Lac pA* 22 24 31.4283564864 +43 43 10.978781916 11.22 10.61 9.69     F7I 115 0
18 HD 235858 pA* 22 29 10.3748806056 +54 51 06.344572284   11.40 9.52 8.47 7.34 G5Ia 264 0
19 IRAS 23304+6147 pA* 23 32 44.7858431592 +62 03 49.090372272   15.36 12.99 12.23 10.50 G2Ia 121 0

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