2019A&A...631A..43M


Query : 2019A&A...631A..43M

2019A&A...631A..43M - Astronomy and Astrophysics, volume 631A43-43 (2019/11-1)

Influence of inelastic collisions with hydrogen atoms on the non-local thermodynamic equilibrium line formation for Fe I and Fe II in the 1D model atmospheres of late-type stars.

MASHONKINA L., SITNOVA T., YAKOVLEVA S.A. and BELYAEV A.K.

Abstract (from CDS):


Context.Iron plays a crucial role in studies of late-type stars.In their atmospheres, neutral iron is the minority species, and lines of FeI are subject to the departures from local thermodynamic equilibrium (LTE).In contrast, one believes that LTE is a realistic approximation for FeII lines. The main source of the uncertainties in the non-LTE (NLTE) calculations for cool atmospheres is a treatment of inelastic collisions with hydrogen atoms.
Aims. Our aim is to investigate the effect of FeI+HI and FeII+HI collisions and their different treatments on the FeI/FeII ionisation equilibrium and iron abundance determinations for three Galactic halo benchmark stars (HD 84937, HD 122563, and HD 140283) and a sample of 38 very metal-poor giants in the dwarf galaxies with well known distances.
Methods. We performed the NLTE calculations for FeI-FeII by applying quantum-mechanical rate coefficients for collisions with HI from recent papers.
Results. We find that collisions with HI serve as efficient thermalisation processes for FeII, to an extent that the NLTE abundance corrections for FeII lines do not exceed 0.02dex, in absolute value, for [Fe/H]≥-3, and reach +0.06dex at [Fe/H]~-4. For a given star, different treatments of FeI+HI collisions lead to similar average NLTE abundances from the FeI lines, although discrepancies in the NLTE abundance corrections exist for individual lines. By using quantum-mechanical collisional data and the Gaia-based surface gravity, we obtain consistent abundances from the two ionisation stages, FeI and FeII, for red giant HD 122563. For turn-off star HD 84937, and subgiant HD 140283, we analyse the iron lines in the visible and the ultra-violet (UV, 1968-2990Å) ranges. For either FeI or FeII, abundances from the visible and UV lines are found to be consistent in each star. The NLTE abundances from the two ionisation stages agree within 0.10dex and 0.13dex for two different treatments of FeI + HI collisions. The FeI/FeII ionisation equilibrium is achieved for each star of our stellar sample in the dwarf galaxies, with the exception of stars at [Fe/H]≤-3.7.

Abstract Copyright: © ESO 2019

Journal keyword(s): atomic processes - stars: abundances - stars: atmospheres - stars: late-type - line: formation

VizieR on-line data: <Available at CDS (J/A+A/631/A43): stars.dat table2.dat table4.dat>

Simbad objects: 48

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Number of rows : 48
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 2MASS J00571020-3328359 Ev* 00 57 10.2179527464 -33 28 35.800377672   18.765 17.798   16.655 ~ 10 0
2 2MASS J00573485-3339457 Ev* 00 57 34.8471871440 -33 39 45.706787496   19.017 18.058   16.962 ~ 9 0
3 [CSF2018] 11-1-4296 Pe* 00 59 38.7626222568 -33 46 14.631963456     19.16   18.04 ~ 10 0
4 [CSF2018] 6-6-402 Ev* 01 00 00.4077384576 -33 29 15.452889144           ~ 8 0
5 [V78] 551 Ev* 01 00 01.1459036832 -33 59 21.358222944           ~ 13 0
6 2MASS J01000496-3401169 Ev* 01 00 05.0225885112 -34 01 16.599373572     18.38   17.19 ~ 8 0
7 NAME Sculptor Dwarf Galaxy G 01 00 09.4 -33 42 32   9.79 8.6 8.81   ~ 1498 4
8 2MASS J01001295-3342038 RG* 01 00 12.9546658464 -33 42 03.847742604   18.96 18.029   16.84 ~ 16 0
9 2MASS J01004244-3343090 RG* 01 00 42.4416724536 -33 43 09.094759788   18.42 16.983   15.576 ~ 16 0
10 2MASS J01004785-3341029 RG* 01 00 47.8436551872 -33 41 03.185910636   19.16 18.187   17.116 ~ 22 0
11 [MFW2011] 24017 Ev* 01 01 22.2460670952 -33 46 21.849866004           ~ 10 0
12 [SHT2013] Scl002 06 Ev* 01 01 26.7622707600 -33 02 59.802667188   18.265 17.120   15.784 ~ 8 0
13 MCG-06-07-001 G 02 39 59.3 -34 26 57   9.02 7.4     ~ 1894 1
14 [BTH2006] fnx-05 042 RG* 02 41 30.9834683776 -33 55 44.764614638           ~ 8 0
15 [FSG2010] UMaII-S1 RG* 08 49 53.4624869976 +63 08 21.677104536           ~ 15 0
16 NAME UMa II Galaxy G 08 51 30.0 +63 07 48     13.3     ~ 410 0
17 [FSG2010] UMaII-S2 RG* 08 52 33.5093638824 +63 05 01.103748900           F5 17 0
18 [FSG2010] UMaII-S3 RG* 08 52 59.0384316768 +63 05 54.601218996           F2 12 0
19 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
20 NAME Sextans dSph LSB 10 13 02.9 -01 36 53   12 10.4     ~ 921 0
21 2MASS J10134175-0211244 RG* 10 13 41.7632659656 -02 11 24.408856392           ~ 14 0
22 [AAS2009] S 24-72 Pe* 10 15 02.6077156167 -01 29 55.016132612           ~ 10 0
23 NAME Leo IV-S1 RG* 11 32 55.9959522600 -00 30 27.821242008           ~ 12 0
24 NAME Leo IV LSB 11 32 57.0 -00 32 00     15.1     ~ 419 1
25 2MASS J13583380+1421083 RB? 13 58 33.8132852928 +14 21 08.488847052           ~ 30 0
26 2MASS J13594880+1419430 RB? 13 59 48.8035332144 +14 19 42.902306436           ~ 12 0
27 [NGW2008] 130 RB? 13 59 48.9735940008 +14 30 06.215943348           ~ 11 0
28 NAME Bootes Dwarf Spheroidal Galaxy G 14 00 00.0 +14 30 00     12.8     ~ 491 0
29 2MASS J14000107+1436515 RB? 14 00 01.0701105384 +14 36 51.510832956           ~ 13 0
30 2MASS J14001049+1431454 RB? 14 00 10.4860038864 +14 31 45.523177176           ~ 20 0
31 2MASS J14001174+1425013 RB? 14 00 11.7235211064 +14 25 01.409650068           ~ 15 0
32 2MASS J14001456+1435527 RB? 14 00 14.5619559384 +14 35 52.725428304           ~ 19 0
33 2MASS J14002582+1426073 RB? 14 00 25.8319555968 +14 26 07.618237800           ~ 16 0
34 2MASS J14003150+1434034 RB? 14 00 31.5041705280 +14 34 03.572360688           ~ 18 0
35 2MASS J14003651+1439272 RB? 14 00 36.5169418536 +14 39 27.331581456           ~ 13 0
36 HD 122563 Pe* 14 02 31.8455084952 +09 41 09.944391876 7.47 7.10 6.19 5.37 4.79 G8:III:Fe-5 920 0
37 2MASS J15020149+6649221 Pe* 15 02 01.4611529376 +66 49 22.389012552     18.07   16.96 ~ 5 0
38 2MASS J15022550+6655249 Pe* 15 02 25.5033321264 +66 55 25.003509816     17.46   16.30 ~ 9 0
39 2MASS J15055198+6641297 Pe* 15 05 52.0087536792 +66 41 29.692521456     16.94   15.59 ~ 12 0
40 2MASS J15081004+6717248 RB? 15 08 10.0432980480 +67 17 24.941562756           ~ 16 0
41 Z 318-18 G 15 09 08.0 +67 13 21   13.60 10.6     ~ 1459 0
42 2MASS J15095749+6709280 RB? 15 09 57.4624658304 +67 09 27.557952552     18.301   17.296 ~ 9 0
43 2MASS J15101168+6708289 RB? 15 10 11.6744038656 +67 08 28.968646272     17.279   15.994 ~ 16 0
44 2MASS J15110089+6653041 RB? 15 11 00.8915042040 +66 53 04.216167924           ~ 12 0
45 Irwin UMi 28104 Pe* 15 13 12.3301392624 +67 33 20.531983896           ~ 15 0
46 2MASS J15132607+6716227 RB? 15 13 26.0756537520 +67 16 22.686607776           ~ 12 0
47 2MASS J15133030+6706368 RB? 15 13 30.2881618176 +67 06 36.839132856           ~ 15 0
48 HD 140283 Pe* 15 43 03.0971190219 -10 56 00.595693188 7.508 7.711 7.212 6.63 8.21 F9VkA5mA1 985 0

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