2023MNRAS.519.5554A


Query : 2023MNRAS.519.5554A

2023MNRAS.519.5554A - Mon. Not. R. Astron. Soc., 519, 5554-5566 (2023/March-2)

The Pristine survey - XX. GTC follow-up observations of extremely metal-poor stars identified from Pristine and LAMOST.

ARENTSEN A., AGUADO D.S., SESTITO F., GONZALEZ HERNANDEZ J.I., MARTIN N.F., STARKENBURG E., JABLONKA P. and YUAN Z.

Abstract (from CDS):

Ultra-metal-poor stars ($\rm {[Fe/H]} \lt -4.0$) are very rare, and finding them is a challenging task. Both narrow-band photometry and low-resolution spectroscopy have been useful tools for identifying candidates, and in this work, we combine both approaches. We cross-matched metallicity-sensitive photometry from the Pristine survey with the low-resolution spectroscopic Large Sky Area Multi-Object Fibre Spectroscopic Telescope (LAMOST) data base, and re-analysed all LAMOST spectra with $\rm {[Fe/H]} _{\rm Pristine} \lt -2.5$. We find that ∼1/3rd of this sample (selected without $\rm {[Fe/H]} _{\rm Pristine}$ quality cuts) also have spectroscopic $\rm {[Fe/H]} \lt -2.5$. From this sample, containing many low signal-to-noise ratio (S/N) spectra, we selected 11 stars potentially having $\rm {[Fe/H]} \lt -4.0$ or $\rm {[Fe/H]} \lt -3.0$ with very high carbon abundances, and we performed higher S/N medium-resolution spectroscopic follow-up with the Optical System for Imaging and low Resolution Integrated Spectroscopy (OSIRIS) on the 10.4-m Gran Telescopio Canarias (GTC). We confirm their extremely low metallicities, with a mean of $\rm {[Fe/H]} = -3.4$, and the most metal-poor star having $\rm {[Fe/H]} = -3.8$. Three of these are clearly carbon-enhanced metal-poor (CEMP) stars with $+1.65 \lt \rm {[C/Fe]} \lt +2.45$. The two most carbon-rich stars are either among the most metal-poor CEMP-s stars or the most carbon-rich CEMP-no stars known, the third is likely a CEMP-no star. We derived orbital properties for the OSIRIS sample and find that only one of our targets can be confidently associated with known substructures/accretion events, and that three out of four inner halo stars have prograde orbits. Large spectroscopic surveys may contain many hidden extremely and ultra-metal-poor stars, and adding additional information from e.g. photometry as in this work can uncover them more efficiently and confidently.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): techniques: spectroscopic - stars: chemically peculiar - stars: Population II - Galaxy: halo

VizieR on-line data: <Available at CDS (J/MNRAS/519/5554): table1.dat table2.dat table3.dat table4.dat>

Simbad objects: 16

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Number of rows : 16
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 LAMOST J002953.07+320229.9 Pe* 00 29 53.0379914456 +32 02 30.141016265           ~ 1 0
2 NAME Sagittarius Stream St* 02 22 +00.0           ~ 1001 0
3 LAMOST J131532.41+121107.4 Pe* 13 15 32.4186146311 +12 11 07.488522768           ~ 1 0
4 Wolf 1492 Pe* 13 40 02.4921849768 -00 02 18.750053436 11.601 11.832 11.451 11.184 10.892 sdF0: 299 0
5 LAMOST J134510.95+424910.8 Pe* 13 45 10.9818188702 +42 49 10.792017117           ~ 1 0
6 LAMOST J142055.86+075308.7 Pe* 14 20 55.8733178017 +07 53 08.761405755           ~ 1 0
7 LAMOST J144714.22+163425.4 Pe* 14 47 14.2384239449 +16 34 25.350703374           ~ 1 0
8 LAMOST J145214.98+160357.6 Pe* 14 52 14.9854906736 +16 03 57.741619842           ~ 1 0
9 LAMOST J145611.30+161925.7 Pe* 14 56 11.3167431655 +16 19 25.864074091           ~ 1 0
10 LAMOST J161021.42+451247.5 Pe* 16 10 21.4295266148 +45 12 47.493006061           ~ 1 0
11 LAMOST J162359.32+303740.8 Pe* 16 23 59.3187712653 +30 37 40.904322535           ~ 1 0
12 LAMOST J212109.07+151328.7 Pe* 21 21 09.0578481878 +15 13 29.041882116           ~ 1 0
13 LAMOST J230209.39+302100.6 Pe* 23 02 09.3943278112 +30 21 00.720055893           ~ 1 0
14 NAME Gaia Enceladus-Sausage St* ~ ~           ~ 860 0
15 NAME Helmi Stream St* ~ ~           ~ 144 0
16 NAME Thamnos Stream St* ~ ~           ~ 63 0

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