Table 11
Central wavelengths from NIST or Kurúcz line lists and total oscillator strengths from line lists by Kurúcz, NIST, and VALD, the literature, and adopted values.
Species | λ (Å) | χex (eV) | g f Kurucz | g f NIST | g f VALD | g f literature | g f adopted | B-107 | B-122 | B-128 | B-130 | ||||||||||
|
|||||||||||||||||||||
EuII | 6437.640 | 1.319712 | −0.276 | – | −0.320 | −0.323 | −0.32 | +0.45 | +0.30 | +0.30 | +0.30 | ||||||||||
EuII | 6645.064 | 1.379816 | +0.204 | – | +0.120 | +0.123 | +0.12 | +0.40 | +0.30 | +0.30 | +0.10 | ||||||||||
BaII | 6141.713 | 0.703636 | −0.076 | 0.0 | −0.076 | −0.076 | 0.00 | +0.40 | 0.0 | +0.50 | +0.10 | ||||||||||
FeI | 6141.730 | 3.602 | −1.60 | – | −1.459 | – | −1.60 | – | – | – | – | ||||||||||
BaII | 6496.897 | 0.604321 | −0.377 | −0.407 | −0.32 | – | −0.32 | +0.50 | +0.10 | +0.60 | +0.35 | ||||||||||
LaII | 6262.287 | 0.403019 | −1.240 | – | −1.220 | −1.222, −1.605 | −1.60 | 0.00 | +0.40 | +0.40 | 0.00 | ||||||||||
LaII | 6320.376 | 0.172903 | −1.610 | – | −1.562 | – | −1.56 | +0.30 | +0.30 | +0.30 | +0.10 | ||||||||||
LaII | 6390.477 | 0.321339 | −1.450 | – | −1.410 | −1.41 | −1.41 | +0.30 | +0.30 | +0.40 | 0.00 | ||||||||||
YII | 5473.388 | 1.738160 | −1.02 | −1.01 | −1.020 | −1.021 | −1.02 | +0.30 | +0.15 | +0.30 | +0.10 | ||||||||||
YII | 5544.611 | 1.738160 | −1.09 | −1.08 | −1.090 | −1.091 | −1.09 | +0.20 | 0.00 | +0.30 | 0.00 | ||||||||||
YII | 5546.009 | 1.748055 | −1.10 | −1.10 | −1.100 | −1.101 | −1.10 | +0.30 | +0.30 | +0.30 | – | ||||||||||
YI | 6435.004 | 0.065760 | −0.820 | −0.83 | −0.820 | −0.821, −1.075 | −0.82 | +0.30 | 0.00 | +0.35 | – | ||||||||||
YII | 6613.733 | 1.011123 | −6.689 | – | −5.587 | – | −5.80 | +0.80 | +1.00 | +1.00 | +0.70 | ||||||||||
FeI | 6613.825 | 1.748055 | −1.110 | −1.110 | −1.110 | −1.111 | −1.15 | – | – | – | – | ||||||||||
YII | 6795.414 | 1.738160 | −1.190 | – | −1.190 | – | −1.19 | 0.00 | 0.00 | +0.30 | +0.10 | ||||||||||
ZrII | 5112.270 | 1.665034 | −0.590 | – | −0.850 | – | −0.59 | 0.00 | +0.10 | +0.40 | 0.00 | ||||||||||
ZrII | 5350.090 | 1.826828 | −1.240 | – | −1.240 | – | −1.24 | – | +0.30 | – | – | ||||||||||
ZrII | 5350.350 | 1.772925 | −1.276 | – | −1.160 | – | −1.16 | +0.30 | +0.30 | – | – | ||||||||||
ZrI | 6127.475 | 0.153855 | −1.06 | – | −1.060 | −1.184, −1.055 | −1.18 | +0.30 | 0.00 | +0.40 | 0.00 | ||||||||||
ZrI | 6134.585 | 0.00 | −1.28 | – | −1.280 | −1.4264, −1.285 | −1.43 | – | 0.00 | +0.35 | – | ||||||||||
ZrI | 6143.252 | 0.070727 | −1.10 | – | −1.100 | −1.2524, −1.105 | −1.50 | – | +0.15 | +0.30 | 0.00 | ||||||||||
SrI | 6503.989 | 2.258995 | +0.26 | −0.05 | +0.320 | – | −0.05 | 0.00 | +0.40 | 0.00 | +0.30 | ||||||||||
SrI | 6791.016 | 1.775266 | −0.720 | −0.73 | −0.73 | – | −0.73 | – | – | +0.40 | – |
Notes. In Col. 7, literature oscillator strength values are taken from the references: and Line-by-line abundances of heavy elements for the four sample stars are given.
Hannaford et al. (1982);
Lawler et al. (2001a);
Lawler et al. (2001b);
Jacobson & Friel (2013);
van der Swaelmen (2013).
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