2012MNRAS.419.2195M


Query : 2012MNRAS.419.2195M

2012MNRAS.419.2195M - Mon. Not. R. Astron. Soc., 419, 2195-2205 (2012/January-3)

Giants reveal what dwarfs conceal: Li abundance in lower red giant branch stars as diagnostic of the primordial Li.

MUCCIARELLI A., SALARIS M. and BONIFACIO P.

Abstract (from CDS):

The discrepancy between cosmological Li abundance inferred from Population II dwarf stars and that derived from big bang nucleosynthesis calculations is still far from being satisfactorily solved. We investigated, as an alternative route, the use of Li abundances in Population II lower red giant branch stars as empirical diagnostic of the cosmological Li. Both theory and observations suggest that the surface Li abundance in metal-poor red giants after the completion of the first dredge-up and before the red giant branch bump is significantly less sensitive to the efficiency of atomic diffusion, compared with dwarf stars. The surface Li abundances in these objects - after the dilution caused by the first dredge-up - are predicted to be sensitive to the total Li content left in the star, i.e. they are affected only by the total amount of Li eventually burned during the previous main-sequence phase. Standard stellar models computed under different physical assumptions show that the inclusion of the atomic diffusion has an impact of about 0.07 dex in the determination of the primordial Li abundance - much smaller than the case of metal-poor main-sequence turnoff stars - and it is basically unaffected by reasonable variations of other parameters (overshooting, age, initial He abundance and mixing length). We have determined from spectroscopy the surface Li content of 17 halo lower red giant branch stars, in the metallicity range between [Fe/H] ∼ - 3.4 and ∼ - 1.4 dex, evolving before the extramixing episode that sets in at the red giant branch bump. The initial Li (customarily taken as estimate of the cosmological Li abundance A(Li)0) has then been inferred by accounting for the difference between initial and post-dredge-up Li abundances in the appropriate stellar models. It depends mainly on the Teff scale adopted in the spectroscopic analysis, and is only weakly sensitive to the efficiency of atomic diffusion in the models, so long as one neglects Li destruction caused by the process competing with atomic diffusion. Our final A(Li)0 estimate spans a relatively narrow range, between 2.28 and 2.46 dex, and is ∼ 0.3-0.4 dex lower than predictions from big bang nucleosynthesis calculations. These values of A(Li)0 are corroborated by the analysis of samples of red giants in the Galactic globular clusters NGC 6397, NGC 6752 and M4. Our result provides an independent quantitative estimate of the difference with the big bang value, and sets a very robust constraint for the physical processes invoked to resolve this discrepancy.

Based on observations collected at the ESO-Very Large Telescope (VLT) under programs 068.D-0546, 072.B-0585, 266.D-5655, 077.D-0018, 65.L-0165 and on data available in the ELODIE archive. This research has also made use of the SIMBAD data base, operated at CDS, Strasbourg, France.


Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

Journal keyword(s): stars: abundances - stars: evolution - stars: Population II - globular clusters: individual: M4 - globular clusters: individual: NGC 6397 - globular clusters: individual: NGC 6752

Simbad objects: 25

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Number of rows : 25
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 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
2 HD 2665 PM* 00 30 45.4469338728 +57 03 53.628989292 8.66 8.51 7.72     G5IIIw 188 0
3 CD-30 298 RG* 00 58 43.8709169280 -30 05 57.717373920   11.43 10.83     F6Vwl 66 1
4 HD 6755 SB* 01 09 43.0577179701 +61 32 50.264076956 8.48 8.40   7.3   G5 252 0
5 CD-24 1782 Pe* 03 38 41.4850201416 -24 02 50.292102948   10.54 9.97 9.246 8.811 ~ 91 0
6 HD 26169 Pe* 04 00 52.4379302184 -75 36 11.436994836 9.58 9.53 8.80 8.51 8.73 G3wpec 88 0
7 HD 27928 SB* 04 22 55.1398810056 -37 15 49.243422348   10.22 9.53     Gw 61 0
8 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
9 HD 274939 Pe* 05 33 17.9573469360 -47 56 13.837114176 10.27 10.15 9.42     G0 63 0
10 HD 45282 Pe* 06 26 40.7720940072 +03 25 29.792391024 8.71 8.69 8.03     Gwl 164 0
11 HD 87140 PM* 10 04 43.1808079344 +54 20 43.425537648 9.70 9.68 8.98     K0 120 0
12 BD-01 2582 RG* 11 53 37.3231720128 -02 00 36.728298108   10.29 9.60     CEMP-s 125 0
13 HD 111721 RG* 12 51 25.1948519215 -13 29 28.166947989   8.78 7.97     G6V 175 0
14 NGC 5139 GlC 13 26 47.28 -47 28 46.1           ~ 3677 0
15 HD 128279 Pe* 14 36 48.5108525999 -29 06 46.612858494 8.64 8.63 8.00     Gw 214 0
16 M 4 GlC 16 23 35.22 -26 31 32.7           ~ 1978 0
17 BD+23 3130 Pe* 17 32 41.6247211304 +23 44 11.625460773     8.9 8.6   G0III 144 0
18 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 2103 0
19 HD 175305 RG* 18 47 06.4416868934 +74 43 31.451436187 8.07 7.93 7.18 6.52 6.03 G5III 239 0
20 M 54 GlC 18 55 03.33 -30 28 47.5           ~ 1164 0
21 NAME SDG G 18 55 19.0 -30 32 43   4.5 3.6     ~ 2438 2
22 NGC 6752 GlC 19 10 52.11 -59 59 04.4           ~ 2121 0
23 HD 200654 Pe* 21 06 34.7513254468 -49 57 50.280288000   9.74 9.1     CEMP 118 0
24 * nu. Ind ** 22 24 36.8853892493 -72 15 19.488237466   5.94 5.29     G9VFe-3.1CH-1.5 290 0
25 HD 218857 Pe* 23 11 24.5948299440 -16 15 04.026507912   9.60 9.0     G5/8w(a) 124 0

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