2015A&A...577A..10B


Query : 2015A&A...577A..10B

2015A&A...577A..10B - Astronomy and Astrophysics, volume 577A10-10 (2015/5-1)

Far-infrared study of K giants in the solar neighborhood: Connection between Li enrichment and mass-loss.

BHARAT KUMAR Y., REDDY B.E., MUTHUMARIAPPAN C. and ZHAO G.

Abstract (from CDS):

A small group of red giant branch (RGB) stars are known to have anomalous Li enhancement whose origin is still not well understood. Some studies have proposed that the Li enhancement in RGB stars is correlated to their far-IR excess, a result of mass loss. Studies to confirm such a correlation have a significant bearing on our understanding of the Galactic Li enhancement. We searched for a correlation between the two anomalous properties of K giants: Li enhancement and IR excess from an unbiased survey of a large sample of RGB stars. A sample of 2000 low-mass K giants with accurate astrometry from the Hipparcos catalog was chosen for which Li abundances have been determined from low-resolution spectra. Far-IR data were collected from the WISE and IRAS catalogs. To probe the correlation between the two anomalies, we supplemented 15 Li-rich K giants discovered from this sample with 25 known Li-rich K giants from other studies. Dust shell evolutionary models and spectral energy distributions were constructed using the code DUSTY to estimate different dust shell properties, such as dust evolutionary time scales, dust temperatures, and mass-loss rates. Among 2000 K giants, we found about two dozen K giants with detectable far-IR excess, and surprisingly, none of them are Li-rich. Similarly, the 15 new Li-rich K giants that were identified from the same sample show no evidence of IR excess. Of the total 40 Li-rich K giants, only 7 show IR excess. Important is that K giants with Li enhancement and/or IR excess begin to appear only at the bump on the RGB.
Result. show that K giants with IR excess are very rare, similar to K giants with Li enhancement. This may be due to the rapid differential evolution of dust shell and Li depletion compared to RGB evolutionary time scales. We also infer from the results that during the bump evolution, giants probably undergo some internal changes, which are perhaps the cause of mass-loss and Li-enhancement events. However, the available observational results do not ascertain that these properties are correlated. That a few Li-rich giants have IR excess seems to be pure coincidence.

Abstract Copyright: ∼

Journal keyword(s): infrared: stars - stars: late-type - circumstellar matter - stars: mass-loss - stars: abundances - stars: evolution

Simbad objects: 41

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Number of rows : 41
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 6665 RG* 01 07 36.4153952208 +20 33 43.304774508   9.65 8.44     G5 25 0
2 HD 8676 * 01 25 18.2208786120 -14 59 38.897293740   8.82 7.75     K0III 21 0
3 V* OP And RG* 01 36 27.2005869192 +48 43 22.000439676   7.47 6.22     K1III: 110 0
4 HD 10437 RG* 01 43 21.4790976792 +59 37 57.933598548   7.65 6.58     K1III 31 0
5 HD 12203 RG* 01 59 58.4062499232 +06 02 07.760309928   7.78 6.76     G5 28 0
6 HD 19745 AB? 03 07 03.2479728720 -65 26 56.811398748   10.16 9.10     K1III 48 0
7 HD 37719 * 05 38 08.9652707304 -47 42 51.433689312   8.70 7.60     K1III 22 0
8 HD 40168 * 05 56 54.7278045696 -08 23 02.504688288   7.90 6.88     K0III 19 0
9 HD 40827 * 06 05 08.2302835584 +59 23 35.569403448   7.442 6.321     K0+IIICN1- 41 0
10 HD 51367 * 06 55 36.4695635136 -33 48 24.617024424   8.14 6.99     K1/2III 18 0
11 HD 63798 RG* 07 50 51.0985296240 +04 27 34.254471600   7.45 6.50     G8III/IV 33 0
12 HD 233517 RG* 08 22 46.7147840400 +53 04 49.230337440   10.85 9.71     K2 98 0
13 HD 77361 PM* 09 01 11.4195560784 -26 39 49.377296592 8.49 7.352 6.187     K1IIICNII 37 0
14 HD 88476 RG* 10 12 42.5357403936 +28 14 31.253650044 8.410 7.790 6.860     ~ 31 0
15 * 35 UMa RG* 10 29 54.4368456192 +65 37 34.432258584   7.463 6.309     K2III: 46 0
16 HD 102845 * 11 50 19.6035126480 -15 51 49.193301420   7.069 6.122     G6III 29 0
17 HD 107484 RG* 12 21 10.0855259160 +41 28 58.909442232   8.89 7.7     K0III 28 0
18 HD 108471 RG* 12 27 42.0816469128 +08 36 37.237288644   7.293 6.342     G8III 51 0
19 HD 112127 C* 12 53 55.7452187592 +26 46 47.982961020 9.56 8.14 6.88 5.97 5.39 C-R4IIIb 169 0
20 * 63 Vir PM* 13 23 01.1146683912 -17 44 06.988406028   6.349 5.354     K0III 70 0
21 IRAS 13313-5838 pA* 13 34 37.4129893008 -58 53 32.360159508     13.15     K5I 24 0
22 HD 118319 V* 13 36 50.5708633872 -34 28 04.217360376   7.497 6.476     K0III 26 0
23 HD 120602 RG* 13 50 24.6787096752 +05 29 49.996860540   6.892 5.993     K0 54 0
24 IRAS 13539-4153 TT* 13 56 57.2669997408 -42 08 09.867862428   14.40 12.80 12.33   K 25 0
25 * 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
26 * 8 UMi * 14 56 48.3523031832 +74 54 03.321176292   7.834 6.835     K0 53 0
27 HD 145457 RG* 16 10 03.9144033672 +26 44 33.893220120   7.61 6.565 6.91   K0III 77 1
28 HD 148293 RG* 16 21 48.7107861744 +69 06 33.814560060   6.376 5.264     K2III 89 0
29 HD 150902 * 16 34 30.1948134456 +77 39 14.215179060   8.98 7.89 7.3   G5 26 0
30 IRAS 17596-3952 LP* 18 03 06.7741393824 -39 51 53.999146152         10.59 ~ 18 0
31 HD 167304 RG* 18 12 42.6145698936 +41 08 48.610387752   7.420 6.352     K0III 32 0
32 HD 170527 RG* 18 25 10.1138252544 +64 50 18.307185756   7.86 6.86     K0 45 0
33 TYC 3105-152-1 RG* 18 36 29.3352012840 +39 04 11.761349916   10.97 9.81     K1III 17 0
34 HD 183492 RG* 19 29 22.1540342928 +14 35 45.669109020   6.618 5.564     K0III 68 0
35 V* V859 Aql LP* 19 31 01.2268057224 +05 23 53.497744980   11.64 10.39     ~ 28 0
36 HD 194937 RG* 20 28 07.5395918472 +08 26 14.813159676   7.290 6.229     G9III 34 0
37 HD 203136 RG* 21 18 40.3832943744 +50 10 56.792571384   8.65 7.73     K0III 29 0
38 * 50 Aqr PM* 22 24 27.0599050724 -13 31 45.731214905   6.717 5.752     G7.5III 51 0
39 HD 214995 RG* 22 41 57.4558645656 +14 30 59.018355504   7.027 5.921     K0III 77 0
40 V* DI Psc RG* 22 59 59.3874643920 +05 09 34.477650828   8.32 7.16     K0III/IV 37 0
41 V* BI Ind RS* 23 13 52.7842528944 -68 17 28.814107128   8.89 7.67     K2IIIp 50 0

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