2022RAA....22g5005X


Query : 2022RAA....22g5005X

2022RAA....22g5005X - Research in Astron. and astroph., 22, part no 7, 5005-5005 (2022/July-~)

Two New r-process-enhanced Stars with [Fe/H] > -0.6 dex from the LAMOST-MRS Survey.

XIE X.-J., SHI J.-R., CHEN T.-L., YAN H.-L., CHEN T.-Y., PAN K.-K., LI C.-Q., LIU S., GAO Q., YAN T.-S. and DING M.-Y.

Abstract (from CDS):

We report the discovery of two r-process-enhanced stars with [Fe/H] > -0.6 dex selected from the Large Sky Area Multi-Object Fiber Spectroscopic Telescope (LAMOST) survey. Three candidate stars have been selected from the LAMOST medium-resolution (R ∼ 7500) spectroscopic survey, and the followed-up high signal-to-noise ratio and high-resolution (R ∼ 31,500) spectra are obtained with the ARC Echelle Spectrograph mounted on the 3.5 m telescope at the Apache Point Observatory, which allow us for the determination of stellar atmospheric parameters and abundances of 20 elements. Among these three r-process-enhanced candidate stars, TYC 1710-933-1 and TYC 2858-372-1 have [Eu/Fe] higher than 0.3 dex and [Ba/Eu] lower than 0.0 dex, thus, can be identified as new r-process-enhanced objects. TYC 2858-372-1 shows similar r+s-process pattern to the Sun. TYC 1710-933-1 presents enhancement of the r-process elements of Nd and Eu. Our work indicates that the enrichment mechanisms of the heavy neutron-capture elements are complicated for metal-rich stars.

Abstract Copyright: © 2022. National Astronomical Observatories

Journal keyword(s): stars: abundances - stars: chemically peculiar - stars: fundamental parameters

Simbad objects: 4

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Number of rows : 4
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 TYC 2858-372-1 * 02 52 40.8779124000 +44 18 02.290015944   12.41 11.39     ~ 1 0
2 HD 33750 * 05 12 59.2462227600 +13 57 52.605035748   9.91 8.83     K0 8 0
3 TYC 3143-542-1 * 19 30 54.5987248536 +41 52 37.481754432   11.76 11.43     F5V 4 0
4 TYC 1710-933-1 * 22 51 45.9157369608 +22 28 19.255678500   13.30 11.88     ~ 1 0

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