2012MNRAS.427...11L


Query : 2012MNRAS.427...11L

2012MNRAS.427...11L - Mon. Not. R. Astron. Soc., 427, 11-26 (2012/November-3)

Lithium abundance in atmospheres of F- and G-type supergiants and bright giants.

LYUBIMKOV L.S., LAMBERT D.L., KAMINSKY B.M., PAVLENKO Y.V., POKLAD D.B. and RACHKOVSKAYA T.M.

Abstract (from CDS):

Lithium in the atmosphere of a F or G supergiant reflects the initial Li abundance and the internal history of the star. During evolution of a star from the main sequence (MS) to the supergiant phase, lithium may be destroyed by, for example, rotationally induced mixing in the MS stars and strongly diluted by development of the supergiant's convective envelope. In order to probe the connection between atmospheric Li abundance and evolutionary predictions, we present a non-local thermodynamic equilibrium abundance analysis of the resonance doublet LiI at 6707.8Å for 55 Galactic F and G supergiants and bright giants (we observed 43 of them, the remaining 12 are added from Luck and Wepfer's list). The derived lithium abundances logε(Li) may be considered in three groups, namely: (i) 10 Li-rich giants with logε(Li) = 2.0–3.2 (all 10 are F-type or A9 stars); (ii) 13 G- to K0-type stars with Li abundances in the narrow range logε(Li) = 1.1–1.8; (iii) all other stars provide just upper limits to the Li abundance.

The derived Li abundances are compared with theoretical predictions of 2–15M☉ stars (both rotating and non-rotating). Our results are generally in good agreement with theory. In particular, the absence of detectable lithium for the majority of programme stars is explainable. The comparison suggests that the stars may be separated by mass M into two groups, namely M ≲ 6M☉ and M > 6M☉. All Li-rich giants and supergiants with logε(Li) ≥ 2.0 have masses M < 6M☉; this conclusion follows not only from our work but also from a scrutiny of published data. 11 of 13 stars with logε(Li) = 1.1–1.8, specifically the stars with M < 6M☉, show good agreement with the post-first dredge-up surface abundance logε(Li) ≈ 1.4 predicted for the non-rotating 2–6M☉ stellar models. An absence of Li-rich stars in the range M > 6M☉ agrees with the theoretical prediction that F and G supergiants and giants with M > 6M☉ cannot show detectable lithium.

We note that present theory appears unable to account for the derived Li abundances for some stars, namely for (i) a few relatively low-mass Li-rich giants (M < 6M☉), whose high Li abundances accompanied by rather high rotational velocities or substantial nitrogen excess contradict theoretical predictions; (ii) the relatively high-mass supergiants HR461 and HR8313 (M > 6M☉) with the detected abundances logε = 1.3–1.5. It is possible that the lithium in such stars was synthesized recently.


Abstract Copyright: © 2012 The Authors Monthly Notices of the Royal Astronomical Society © 2012 RAS

Journal keyword(s): stars: abundances - stars: evolution - supergiants

Simbad objects: 58

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Number of rows : 58
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 * 36 Psc ** 00 16 34.0418564136 +08 14 24.566106696   7.042 6.121     G8II-III 60 0
2 HD 3421 * 00 37 21.2197453944 +35 23 58.210707084   6.323 5.431     G2Ib-II 87 0
3 HD 4362 * 00 46 42.4584874152 +59 34 28.347458772   7.463 6.410     G0Ibe 86 0
4 HD 9900 * 01 38 07.5665016360 +57 58 39.475310304   6.921 5.536     K0II_CN+2 77 0
5 HD 16780 * 02 43 01.8568506264 +48 15 54.878632596 8.310 7.430 6.280     G5II 30 0
6 HD 17818 * 02 53 21.0706663824 +48 34 11.848899324 8.390 7.420 6.210     G8II 35 0
7 HD 17905 * 02 53 24.3726613608 +31 38 40.858465488   7.12 6.60     F6II-III 39 0
8 * nu. Per * 03 45 11.6327358410 +42 34 42.709540671 4.50 4.22 3.80 3.40 3.13 F4II 136 0
9 HD 25291 * 04 04 27.1629402984 +59 09 19.832668272 6.10 5.63 5.12 4.62 4.24 F0II 115 0
10 HD 25877 * 04 09 27.5710891104 +59 54 29.052740304   7.407 6.295     G7II 64 0
11 * omi01 Eri dS* 04 11 51.9390483214 -06 50 15.286647564   4.357 4.026     F0III 159 0
12 * mu. Per SB* 04 14 53.8635146524 +48 24 33.590334394 5.75 5.12 4.16 3.38 2.83 G0Ib 252 0
13 HD 27022 * 04 20 40.3256358240 +65 08 25.589310792 6.55 6.08 5.27 4.63 4.20 G4III 160 0
14 * bet Cam * 05 03 25.0910670105 +60 26 32.083933247 5.57 4.95 4.02 3.33 2.86 G1Ib 190 0
15 HD 32655 * 05 06 49.5553255488 +43 10 28.940916900   6.646 6.207     F0IIIa 61 0
16 * bet Lep PM* 05 28 14.7228880318 -20 45 33.997988694 4.13 3.66 2.84 2.19 1.75 G5II-IIIa: 254 0
17 HD 38713 * 05 47 07.8044115888 -16 14 17.086172172   7.058 6.157     G8III 36 0
18 * 25 Gem * 06 41 20.8975543776 +28 11 47.904494928   7.521 6.427     G5Ib 97 0
19 * del CMa s*y 07 08 23.4840514 -26 23 35.518484 3.06 2.52 1.84 1.33 1.00 F8Ia 348 0
20 HD 57146 * 07 18 51.2737383648 -26 35 09.081112236   6.258 5.288     G2Ib 86 0
21 HD 58526 * 07 25 51.1999347000 -05 46 29.862957504   6.895 5.962     G3Ib 68 0
22 HD 59890 * 07 30 42.6019759200 -30 57 44.209928016 6.21 5.58 4.65 3.98 3.51 G2Iab/b 68 0
23 HD 61295 PM* 07 39 54.0948913920 +32 00 35.034156612   6.523 6.165     F5III 62 0
24 * ksi Pup * 07 49 17.6535518440 -24 51 35.221966694 5.72 4.56 3.30 2.43 1.88 G6Ib 201 0
25 * j Pup * 07 56 51.5423244834 -22 52 48.401855869   4.900 4.184     F7II 114 0
26 * zet Mon * 08 08 35.6480975954 -02 59 01.635577977 6.02 5.30 4.33 3.60 3.11 G2Ib 152 0
27 * 55 Cam Pe* 08 12 48.7881816720 +68 28 26.663711052   6.352 5.329     G7IIb 112 0
28 * 20 Pup * 08 13 19.9671571968 -15 47 17.608829604 6.84 6.06 4.99     G4Ib-II 90 0
29 HD 71115 * 08 25 54.7670593176 +07 33 52.214573088   6.051 5.122     G6III-IIIaFe-1.5 82 0
30 * F Hya * 08 43 40.3744846779 -07 14 01.422508229   5.441 4.625     G1Ib 172 0
31 HD 76494 * 08 56 37.0374423504 +04 14 11.690050164   7.128 6.131     G8III 42 0
32 * 37 LMi * 10 38 43.2128104658 +31 58 34.463378806   5.494 4.677     G2.5IIIa 162 0
33 * bet Crv PM* 12 34 23.2349224335 -23 23 48.336778328 4.17 3.52 2.64 2.03 1.59 G5IIBa0.3 272 0
34 HD 119035 PM* 13 40 15.5778600264 +31 00 43.328600784   7.17 6.20     G8II-III 46 0
35 * 83 Vir * 13 44 29.8268293824 -16 10 44.662210068   6.350 5.567     G0II: 93 0
36 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
37 HD 142357 * 15 53 34.8696799896 +16 04 29.761652748 6.660 6.630 6.220     F5.5IV+ 62 0
38 * bet Dra * 17 30 25.9616959 +52 18 04.999351 4.43 3.79 2.81 2.12 1.64 G2Ib-IIa 428 0
39 HD 161149 * 17 43 22.0226907336 +14 17 42.610199172   6.643 6.211     F5III 78 0
40 * nu. Her LP* 17 58 30.1496073102 +30 11 21.387652276 4.95 4.80 4.41 4.01 3.78 kA9hF2mF2(IV) 186 0
41 * d Dra * 18 32 34.5225933264 +57 02 44.145773628   5.380 4.761     F8Ib-II 149 0
42 HD 172365 RG* 18 39 36.8773335936 +05 15 51.448369824 6.92 7.15 6.40     F8II 136 0
43 HD 176123 * 18 59 26.7781362168 -18 33 59.166247104   7.358 6.378     G3II 46 0
44 HD 185018 * 19 36 52.4545556280 +11 16 23.522333484   6.834 5.975     G0Ib-II 73 0
45 HD 187203 * 19 48 30.5141801256 +10 41 38.749809156 8.01 7.377 6.457     F8Ib-II 94 0
46 * 35 Cyg SB* 20 18 39.0719928336 +34 58 57.973987704 6.29 5.803 5.162     F6Ib 138 0
47 HD 194069 SB* 20 22 03.0552303672 +41 07 55.691984064   7.409 6.383     G9Ib-II 59 0
48 * gam Cyg V* 20 22 13.7018357 +40 15 24.044963 3.44 2.90 2.23 1.74 1.40 F8Ib 607 0
49 * 41 Cyg V* 20 29 23.7355334165 +30 22 06.799052288 4.69 4.42 4.01 3.65 3.42 F5Ib-II 194 0
50 * 44 Cyg * 20 30 59.2290678096 +36 56 09.023582544 7.93 7.160 6.216 6.90 4.64 F5Ib 161 0
51 * 49 Cyg ** 20 41 02.5422151056 +32 18 26.238680208   6.672 5.638     G8IIb 89 0
52 * bet Aqr * 21 31 33.5320760349 -05 34 16.229381029 4.27 3.71 2.89 2.29 1.84 G0Ib 463 0
53 * 9 Peg V* 21 44 30.6958020785 +17 21 00.062899998 6.48 5.52 4.35 3.53 2.98 G5Ib 274 0
54 HD 209693 * 22 04 34.5174239880 +32 56 30.285443256   7.436 6.370     G5Ib-II 37 0
55 * alf Aqr * 22 05 47.0355458275 -00 19 11.463439527 4.65 3.90 2.94 2.27 1.76 G2Ib 451 0
56 HD 216206 * 22 50 10.0938802752 +50 40 36.908660604   7.336 6.230     G5Ib-II 67 0
57 HD 216756 PM* 22 55 02.6473045344 +37 04 36.582079476   6.295 5.901     F4V 103 0
58 NAME Galactic Bulge reg ~ ~           ~ 4794 0

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