2017ApJ...847..142E


Query : 2017ApJ...847..142E

2017ApJ...847..142E - Astrophys. J., 847, 142-142 (2017/October-1)

Ultra-metal-poor stars: spectroscopic determination of stellar atmospheric parameters using iron Non-LTE line abundances.

EZZEDDINE R., FREBEL A. and PLEZ B.

Abstract (from CDS):

We present new ultra-metal-poor stars parameters with [Fe/H] < -4.0 based on line-by-line non-local thermodynamic equilibrium (NLTE) abundances using an up-to-date iron model atom with a new recipe for non-elastic hydrogen collision rates. We study the departures from LTE in their atmospheric parameters and show that they can grow up to ∼1.00 dex in [Fe/H], ∼150 K in Teff and ∼0.5 dex in log g toward the lowest metallicities. Accurate NLTE atmospheric stellar parameters, in particular [Fe/H] being significantly higher, are the first step to eventually providing full NLTE abundance patterns that can be compared with Population III supernova nucleosynthesis yields to derive properties of the first stars. Overall, this maximizes the potential of these likely second-generation stars to investigate the early universe and how the chemical elements were formed.

Abstract Copyright: © 2017. The American Astronomical Society. All rights reserved.

Journal keyword(s): line: formation - stars: abundances - stars: atmospheres - stars: fundamental parameters - stars: Population II - stars: Population II

VizieR on-line data: <Available at CDS (J/ApJ/847/142): table1.dat table3.dat>

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 CD-38 245 Pe* 00 46 36.1954514592 -37 39 33.555030480   12.733 11.929 13.39 10.996 KIIvw 224 0
2 HE 0057-5959 Pe* 00 59 53.9857261680 -59 43 29.745171408   16.4       CEMP-no 32 0
3 HE 0107-5240 Pe* 01 09 29.1555567432 -52 24 34.202039148   15.89 15.07 15.10 14.283 CEMP-no 244 0
4 SDSS J014036.21+234458.1 Pe* 01 40 36.2207485632 +23 44 58.206182748   15.6       CEMP-no 35 0
5 HE 0233-0343 Pe* 02 36 29.7931635456 -03 30 06.029112888   15.867 15.430 15.171 14.818 CEMP-no 32 0
6 UCAC4 115-002803 Pe* 03 13 00.3747928560 -67 08 39.336144504   15.442 14.753 14.639   CEMP-no 109 0
7 G 77-61 Pe* 03 32 38.0920129269 +01 58 00.084645962   15.60 13.90 12.9   dC-J_CH5 132 0
8 2MASS J05583926-4839567 Pe* 05 58 39.2660594064 -48 39 56.890252404   16.16 15.45 14.991   CEMP-no 88 0
9 HD 84937 Pe* 09 48 56.0992891997 +13 44 39.326709913 8.49 8.68 8.32 7.97 7.70 F8Vm-5 795 0
10 UCAC3 215-112497 Pe* 10 29 15.1489854864 +17 29 27.924626724         15.98 sdA 106 0
11 SDSS J103556.11+064143.9 Pe* 10 35 56.1158830560 +06 41 44.004045912           CEMP-no 26 0
12 SDSS J120441.38+120111.5 Pe* 12 04 41.3884587048 +12 01 11.514049212           A0 16 0
13 2MASS J13132688-0019415 Pe* 13 13 26.8884339336 -00 19 41.336280264           CEMP-no 33 0
14 HE 1310-0536 Pe* 13 13 31.1856437856 -05 52 12.533926152   15.055 14.347 13.829   CEMP-no 30 0
15 HE 1327-2326 Pe* 13 30 05.9394958608 -23 41 49.699340844 13.761 14.01 13.55 13.50 12.803 CEMP-no 245 0
16 Wolf 1492 Pe* 13 40 02.4921849768 -00 02 18.750053436 11.601 11.832 11.451 11.184 10.892 sdF0: 284 0
17 * 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 2318 1
18 HE 1424-0241 Pe* 14 26 40.3306297920 -02 54 27.487168164   15.892 15.45 14.887 14.54 ~ 38 0
19 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 937 0
20 SDSS J174259.67+253135.8 Pe* 17 42 59.6805182976 +25 31 35.892397632           CEMP-no 22 0
21 2MASS J20452353-2842359 Pe* 20 45 23.5333400256 -28 42 35.912310048   14.89 14.03 13.328 12.844 ~ 34 0
22 HE 2139-5432 Pe* 21 42 42.4478261040 -54 18 42.968447028   15.9       CEMP-no 32 0
23 SDSS J220924.74-002859.8 Pe* 22 09 24.7445091576 -00 28 59.826627156           CEMP-no 12 0
24 2MASS J22422683-5004009 Pe* 22 42 26.8476804960 -50 04 00.914721852   16.239 15.846 15.576 15.240 CEMP-mp 16 0
25 HE 2323-0256 Pe* 23 26 29.8073738880 -02 39 58.036383180   15.12 14.36   13.358 CEMP-no 180 0

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