2012A&A...538A..68P


Query : 2012A&A...538A..68P

2012A&A...538A..68P - Astronomy and Astrophysics, volume 538A68-68 (2012/2-1)

Weak G-band stars on the H-R diagram: clues to the origin of the Li anomaly.

PALACIOS A., PARTHASARATHY M., BHARAT KUMAR Y. and JASNIEWICZ G.

Abstract (from CDS):

Weak G-band (WGB) stars are a rare class of cool luminous stars that present a strong depletion in carbon, but also lithium abundance anomalies that have been little explored in the literature since the first discovery of these peculiar objects in the early 1950s. Here we focus on the Li-rich WGB stars and report on their evolutionary status. We explored different paths to propose a tentative explanation for the lithium anomaly. Using archive data, we derived the fundamental parameters of WGB (Teff, logg, log(L/L☉)) using Hipparcos parallaxes and recent temperature scales. From the equivalent widths of Li resonance line at 6707Å, we uniformly derived the lithium abundances and applied NLTE corrections when possible following the procedure described by Lind et al. (2009A&A...503..541L). We also computed dedicated stellar evolution models in the mass range 3.0 to 4.5M☉, exploring the effects of rotation-induced and thermohaline mixing. These models are used to locate the WGB stars in the H-R diagram and to explore the origin of the abundance anomalies. The location of WGB stars in the Hertzsprung-Russell diagram shows that these are intermediate mass stars of masses ranging from 3.0 to 4.5M☉ located at the clump, which implies a degeneracy of their evolutionary status between subgiant/red giant branch and core helium burning phases. The atmospheres of a large proportion of WGB stars (more than 50%) exhibit lithium abundances A(Li)≥1.4dex similar to Li-rich K giants. However, the position of WGB stars along with the Li-rich K giants in the H-R diagram, indicates that both are well-separated groups. The combined and tentatively consistent analysis of the abundance pattern for lithium, carbon, and nitrogen of WGB stars seems to indicate that carbon underabundance could be decorrelated from the lithium and nitrogen overabundances.

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Journal keyword(s): stars: evolution - stars: abundances - stars: late-type - stars: carbon

Simbad objects: 30

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Number of rows : 30
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 HD 16634 * 02 38 30.9879946800 -44 42 27.614795652   8.83 7.83     G5 17 0
2 HD 18636 * 02 58 33.4752514512 -37 59 32.316945756   8.53 8.60     G5III:CN-1CH-4 33 0
3 HD 18474 * 02 59 49.7897133000 +47 13 14.567181096   6.348 5.485     G5:III:CN-3CH-2Hdel-1 116 0
4 HD 21018 SB* 03 23 38.9895882648 +04 52 55.570317168 7.91 7.36 6.50 5.83 5.34 G2III:CH-1: 91 0
5 HD 26575 * 04 10 45.8710071288 -35 16 25.636934100 8.47 7.51 6.44 5.61 5.05 K0IIICN-0.5CH-2 46 0
6 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
7 HD 28932 * 04 33 31.6780613304 +01 01 20.906741748   8.94 7.94     G6III:CH-3 23 0
8 HD 31274 * 04 52 02.0066896512 -46 51 08.783341704 8.87 8.09 7.13 6.36 5.84 K0IIICN-1CH-3.5 36 0
9 HD 31869 * 04 58 11.2603297512 -28 02 08.402208468   10.18 10.00     G8/K1IIICNVp 12 0
10 HD 36552 * 05 30 19.6610664960 -43 41 37.968522828 9.46 8.94 8.08 7.37 6.89 G7III:CN-1CH-2.5 22 0
11 HD 40402 * 05 57 18.9344941656 -27 19 53.425923636 10.20 9.54 8.61 7.87 7.35 G8/K0IIICNVp 35 0
12 HD 49960 * 06 49 40.5443139312 -31 15 32.849109252 10.22 9.37 8.35 7.54 6.95 K2/3IIIp+(G) 23 0
13 HD 56438 * 07 14 36.4077591456 -47 08 05.811480672 10.01 9.14 8.10 7.23 6.59 K0.5IIIbCH-0.5 31 0
14 HD 67728 ** 08 08 37.6489217232 -19 50 23.659349244 9.66 8.66 7.54 6.67 6.07 G8/K0III 34 0
15 HD 78146 * 09 05 44.2117912368 -28 04 59.419602876 10.82 9.72 8.56 7.65 7.00 K1IIICNIV/Vp 33 0
16 HD 82595 * 09 31 57.7827309960 -36 51 34.326602028 10.15 9.21 8.18 7.36 6.80 K2II/III 24 0
17 HD 91805 PM* 10 35 10.4125079496 -43 39 52.512284124 7.75 7.04 6.10 5.32 5.32 G7IIICH-3 49 0
18 HD 94956 * 10 57 23.9921795256 -29 16 50.727621612 10.14 9.41 8.45 7.64 7.12 K0IIICNVp 34 0
19 HD 102851 * 11 50 16.3991537904 -51 28 14.306373372 10.74 9.84 8.77 7.92 7.31 K0/1IIICNVp 23 0
20 HD 119256 * 13 43 36.2761437624 -57 35 23.906631588 9.39 8.45 7.34 6.39 5.72 K1III 23 0
21 HD 120170 * 13 47 58.7910974760 -08 47 22.712626032 10.64 9.97 9.04 9.04 9.04 G8V 24 0
22 HD 120213 * 13 55 38.8756448856 -82 39 58.287116448 8.98 7.39 5.94 5.94 5.94 K2III:CN-1CH-2.5 30 0
23 HD 124721 * 14 16 24.5579949048 -45 11 23.161906824 11.73 10.89 9.85 9.85 9.85 K1/2(III) 19 0
24 HD 146116 * 16 14 38.3963169528 -00 23 55.500437616 9.65 8.75 7.68 6.83 6.20 G7IIICH-2Hdel-0.5 24 0
25 HD 165462 * 18 06 07.4279590896 -00 26 46.059359028 8.16 7.40 6.34     G9IIICH-3 60 0
26 HD 166208 SB* 18 07 28.7442485448 +43 27 42.802503948   5.915 4.997     G8IIICN-1CH-3 160 0
27 HD 165634 * 18 08 04.9788127934 -28 27 25.533540057 6.26 5.51 4.56 3.85 3.32 G7:IIIbCN-1CH-3.5HK+1 105 0
28 HD 188328 ** 19 54 01.95884 +15 17 31.5151           F8III 52 0
29 HD 204046 * 21 26 54.1300999560 -33 54 35.663524020   10.10 9.05     G8/K0IIICNVp 15 0
30 HD 207774 * 21 51 33.5835096192 -07 24 14.303125944   9.85 8.90     G8III 17 0

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