2021ApJ...913L...4S


Query : 2021ApJ...913L...4S

2021ApJ...913L...4S - Astrophys. J., 913, L4-L4 (2021/May-3)

Tracking the evolution of lithium in giants using asteroseismology: super-Li-rich stars are almost exclusively young red-clump stars.

SINGH R., REDDY B.E., CAMPBELL S.W., KUMAR Y.B. and VRARD M.

Abstract (from CDS):

We report novel observational evidence on the evolutionary status of lithium-rich giant stars by combining asteroseismic and lithium abundance data. Comparing observations and models of the asteroseismic gravity-mode period spacing ΔΠ1, we find that super-Li-rich giants (SLRs, A(Li) > 3.2 dex) are almost exclusively young red-clump (RC) stars. Depending on the exact phase of evolution, which requires more data to refine, SLR stars are either (i) less than ∼2 Myr or (ii) less than ∼40 Myr past the main core helium flash (CHeF). Our observations set a strong upper limit for the time of the inferred Li-enrichment phase of <40 Myr post-CHeF, lending support to the idea that lithium is produced around the time of the CHeF. In contrast, the more evolved RC stars (>40 Myr post-CHeF) generally have low lithium abundances (A(Li) <1.0 dex). Between the young, super-Li-rich phase, and the mostly old, Li-poor RC phase, there is an average reduction of lithium by about 3 orders of magnitude. This Li destruction may occur rapidly. We find the situation to be less clear with stars having Li abundances between the two extremes of super-Li-rich and Li-poor. This group, the "Li-rich" stars (3.2 > A(Li) > 1.0 dex), shows a wide range of evolutionary states.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Stellar abundances - Asteroseismology - Stellar interiors - Low mass stars

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 UCAC4 652-066332 * 18 58 31.3580462304 +40 17 36.792659616   13.928 12.558 12.224   K1.5III 15 0
2 BD+44 3032 RG* 18 59 29.1710361672 +45 07 57.583590132   10.39 9.34     K0 16 0
3 TYC 3550-223-1 HB* 19 07 30.9607680312 +50 00 57.460449636   10.85 9.78     G9.5III 28 0
4 2MASS J19091067+4316190 HB* 19 09 10.6701980640 +43 16 18.999496164           K2III 34 0
5 2MASS J19091874+4234532 HB* 19 09 18.7408353600 +42 34 53.281448976           G6V 34 0
6 TYC 3550-1536-1 HB* 19 09 53.6249341080 +48 46 32.531541168   13.13 12.09     K2III 30 0
7 2MASS J19103277+4203166 HB* 19 10 32.7835512144 +42 03 16.501466448           K0III 27 0
8 TYC 3542-1885-1 RG* 19 18 16.4670376200 +45 06 52.645070304   12.40 11.19     K0III 38 0
9 TYC 3133-401-2 Er* 19 19 10.1787880656 +43 45 56.702049552   11.88 10.86     K1.5III 22 0
10 UCAC4 674-070673 RG* 19 20 09.8238737664 +44 44 34.887974604   14.183 12.901 12.653   G6V 19 0
11 2MASS J19202208+4942450 RG* 19 20 22.0937618640 +49 42 44.945912268           ~ 9 0
12 TYC 3555-1010-1 RG* 19 20 30.9424259784 +52 03 28.940388444   12.00 11.10     G8.5IIIb 19 0
13 TYC 3146-218-1 RG* 19 24 06.9388868496 +44 23 22.340539032   12.81 10.88     K1IV 31 0
14 2MASS J19301726+3852008 RG* 19 30 17.2558848240 +38 52 00.848457264           G3III 9 0
15 UCAC4 684-068189 HB* 19 31 54.9293978280 +46 39 57.117241440   13.829 12.519 12.161   K2III 30 0
16 UCAC4 667-075648 HB* 19 33 21.4665101064 +43 12 51.595453044   13.948 12.887 12.568   K0III 24 0
17 TYC 3564-1558-1 HB* 19 36 33.9396770568 +49 38 35.035521396   11.99 11.30     G9.5III 30 0
18 UCAC4 669-075530 RG* 19 38 48.7360722288 +43 38 59.415903852   14.870 13.610 13.260   G8III 21 0
19 2MASS J19422465+4241050 * 19 42 24.6478958232 +42 41 05.017041420           ~ 7 0
20 UCAC4 684-072128 HB* 19 51 40.3673089560 +46 47 28.061128104   13.508 12.451 12.217   G8III 26 0
21 2MASS J19520545+4640204 HB* 19 52 05.4606936792 +46 40 20.478909612           K1IV 27 0
22 UCAC4 682-073002 RG* 19 52 44.7061556400 +46 21 44.863784928   14.696 13.351 13.054   ~ 25 0

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