2017ApJ...835...90Z


Query : 2017ApJ...835...90Z

2017ApJ...835...90Z - Astrophys. J., 835, 90-90 (2017/January-3)

NLTE analysis of high-resolution H-band spectra. II. Neutral magnesium.

ZHANG J., SHI J., PAN K., ALLENDE PRIETO C. and LIU C.

Abstract (from CDS):

Aiming at testing the validity of our magnesium atomic model and investigating the effects of non-local thermodynamical equilibrium (NLTE) on the formation of the H-band neutral magnesium lines, we derive the differential Mg abundances from selected transitions for 13 stars either adopting or relaxing the assumption of local thermodynamical equilibrium (LTE). Our analysis is based on high-resolution and high signal-to-noise ratio H-band spectra from the Apache Point Observatory Galactic Evolution Experiment (APOGEE) and optical spectra from several instruments. The absolute differences between the Mg abundances derived from the two wavelength bands are always less than 0.1 dex in the NLTE analysis, while they are slightly larger for the LTE case. This suggests that our Mg atomic model is appropriate for investigating the NLTE formation of the H-band Mg lines. The NLTE corrections for the Mg I H-band lines are sensitive to the surface gravity, becoming larger for smaller log g values, and strong lines are more susceptible to departures from LTE. For cool giants, NLTE corrections tend to be negative, and for the strong line at 15765 Å they reach -0.14 dex in our sample, and up to -0.22 dex for other APOGEE stars. Our results suggest that it is important to include NLTE corrections in determining Mg abundances from the H-band Mg I transitions, especially when strong lines are used.

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

Journal keyword(s): line: formation - line: profiles - stars: abundances - stars: atmospheres - stars: atmospheres

Simbad objects: 15

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Number of rows : 15
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 * 86 Peg RG* 00 05 41.9616132456 +13 23 46.565281644   6.439 5.537     G5III 79 0
2 * mu. Cas SB* 01 08 16.3029454473 +54 55 12.561201263 5.93 5.86 5.17 4.55 4.13 G5Vb 593 1
3 * 44 And PM* 01 10 18.7404097416 +42 04 53.309986932   6.249 5.665     F8V 194 0
4 HD 22675 RG* 03 38 29.2528166112 -07 23 30.701131116   6.837 5.849     G8.5IIIb 60 0
5 HD 31501 PM* 04 57 59.3728197659 +34 16 04.866504673   8.94   7.7   G8V 88 0
6 * eps CMi * 07 25 38.8996839840 +09 16 33.925520604   5.990 4.986     G6IIb 113 0
7 * 55 Cam Pe* 08 12 48.7881816720 +68 28 26.663711052   6.352 5.329     G7IIb 112 0
8 * bet Vir PM* 11 50 41.7185158616 +01 45 53.001539131 4.26 4.15 3.60 3.13 2.85 F9V 973 0
9 HD 103095 Pe* 11 52 58.7673387755 +37 43 07.254113125 7.38 7.20 6.45 5.80 5.35 K1V_Fe-1.5 842 1
10 * eta Boo SB* 13 54 41.07892 +18 23 51.7946 3.440 3.250 2.680 2.24 1.95 G0IV 733 0
11 * 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 2417 1
12 HD 148816 PM* 16 30 28.4586254384 +04 10 41.602836534 7.75 7.81 7.28 6.82 6.49 F7V 329 0
13 * 49 Dra * 19 00 43.4564400648 +55 39 29.883053808   6.368 5.513     G6IIbFe-0.5 64 0
14 NAME Galactic Bar reg ~ ~           ~ 1458 0
15 NAME Galactic Bulge reg ~ ~           ~ 4794 0

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