2018ApJ...852L..31L


Query : 2018ApJ...852L..31L

2018ApJ...852L..31L - Astrophys. J., 852, L31-L31 (2018/January-2)

Enormous Li enhancement preceding red giant phases in low-mass stars in the Milky Way halo.

LI H., AOKI W., MATSUNO T., KUMAR Y.B., SHI J., SUDA T. and ZHAO G.

Abstract (from CDS):

Li abundances in the bulk of low-mass metal-poor stars are well reproduced by stellar evolution models adopting a constant initial abundance. However, a small number of stars have exceptionally high Li abundances, for which no convincing models have been established. We report on the discovery of 12 very metal-poor stars that have large excesses of Li, including an object having more than 100 times higher Li abundance than the values found in usual objects, which is the largest excess in metal-poor stars known to date. The sample is distributed over a wide range of evolutionary stages, including five unevolved stars, showing no clear abundance anomaly in other elements. The results indicate the existence of an efficient process to enrich Li in a small fraction of low-mass stars at the main-sequence or subgiant phase. The wide distribution of Li-rich stars along the red giant branch could be explained by the dilution of surface Li by mixing that occurs when the stars evolve into red giants. Our study narrows down the problem to be solved in order to understand the origins of Li excess found in low-mass stars, suggesting the presence of an unknown process that affects the surface abundances preceding red giant phases.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): nuclear reactions, nucleosynthesis, abundances - stars: abundances - stars: evolution - stars: low-mass - stars: Population II - stars: Population II

Simbad objects: 22

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Number of rows : 22
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 2796 Pe* 00 31 16.9147531152 -16 47 40.790991624 9.58 9.28 8.50 8.14 8.67 Fw 203 0
2 TYC 647-363-1 Pe* 03 02 09.3287650056 +13 56 56.347501524   13.00 12.24     ~ 4 0
3 UCAC4 713-040958 Pe* 05 54 08.5305002483 +52 35 59.348356258   14.531 13.751 13.497   ~ 8 0
4 UCAC4 753-042171 Pe* 06 26 47.8639498630 +60 32 54.378925263   14.626 13.946 13.889   ~ 6 0
5 UCAC4 580-035854 Pe* 07 05 42.3038780016 +25 52 26.882410182   14.198 13.496 13.432   ~ 9 0
6 TYC 1346-877-1 Pe* 07 14 22.6363616160 +16 00 42.505716312   12.24 11.60     ~ 12 0
7 UCAC4 558-043026 Pe* 07 41 02.0658780670 +21 32 46.931885079       14.045   ~ 7 0
8 UCAC4 686-049450 Pe* 07 58 16.3981269241 +47 03 43.321360032   15.169 14.582 13.904   ~ 8 0
9 UCAC4 583-043587 Pe* 08 52 08.0757656860 +26 27 30.222260775   15.578 15.026 15.085   ~ 5 0
10 HD 84937 Pe* 09 48 56.0992891997 +13 44 39.326709913 8.49 8.68 8.32 7.97 7.70 F8Vm-5 831 0
11 UCAC2 37720962 Pe* 11 49 03.3074623848 +16 58 41.334638376           CEMP-r/s 16 1
12 M 68 GlC 12 39 27.98 -26 44 38.6     7.96     ~ 1069 0
13 UCAC4 639-047150 Pe* 13 14 57.7665995611 +37 41 10.686614709   14.164 13.725 13.578   ~ 7 0
14 NGC 5053 GlC 13 16 27.09 +17 42 00.9     9.96     ~ 675 0
15 2MASS J14141226+0016187 Pe* 14 14 12.2708870112 +00 16 18.754014432   14.35       ~ 6 0
16 UCAC4 515-057600 Pe* 14 55 00.0420842188 +12 51 06.220965541   14.270 13.439 13.400   ~ 4 0
17 NGC 5897 GlC 15 17 24.40 -21 00 36.4   10.16 8.52     ~ 424 0
18 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 985 0
19 NGC 6397 GlC 17 40 42.09 -53 40 27.6     5.17     ~ 2103 0
20 HD 186478 SB* 19 45 14.1409752672 -17 29 27.071239056   10.116 9.302 8.527 7.961 K2III 166 0
21 UCAC4 588-126769 Pe* 21 46 10.1255882832 +27 32 00.727492992   14.88 14.16 14.09   ~ 2 0
22 BPS CS 22893-0010 Pe* 22 58 11.7253311672 -11 56 45.431946204   15.34 14.73 14.70   ~ 19 0

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