2016ApJ...833..137Z


Query : 2016ApJ...833..137Z

2016ApJ...833..137Z - Astrophys. J., 833, 137-137 (2016/December-3)

NLTE analysis of high-resolution H-band spectra. I. Neutral silicon.

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

Abstract (from CDS):

We investigated the reliability of our silicon atomic model and the influence of non-local thermodynamical equilibrium (NLTE) on the formation of neutral silicon (Si i) lines in the near-infrared (near-IR) H-band. We derived the differential Si abundances for 13 sample stars with high-resolution H-band spectra from the Apache Point Observatory Galactic Evolution Experiment (APOGEE), as well as from optical spectra, both under local thermodynamical equilibrium (LTE) and NLTE conditions. We found that the differences between the Si abundances derived from the H-band and from optical lines for the same stars are less than 0.1 dex when the NLTE effects are included, and that NLTE reduces the line-to-line scatter in the H-band spectra for most sample stars. These results suggest that our Si atomic model is appropriate for studying the formation of H-band Si lines. Our calculations show that the NLTE corrections of the Si i H-band lines are negative, i.e., the final Si abundances will be overestimated in LTE. The corrections for strong lines depend on surface gravity, and tend to be larger for giants, reaching ∼-0.2 dex in our sample, and up to ∼-0.4 dex in extreme cases of APOGEE targets. Thus, the NLTE effects should be included in deriving silicon abundances from H-band Si i lines, especially for the cases where only strong lines are available.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

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

Simbad objects: 13

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Number of rows : 13
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

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