Table G.3
Effective principal quantum numbers n*, and ABO theory broadening data, for high-quality lines of neutral species, which are not included in Barklem et al. (2000b).
| Z | El | Wavelength |  |
 |
σ | α | |
|---|---|---|---|---|---|---|---|
| (Å) | ( ) |
||||||
| 6 | C | 6587.6100 | 2.23 | 4.02 | 1953 | 0.320 | |
| 6 | C | 8727.1260 | 1.17 | 1.26 | 154 | 0.266 | a |
| 14 | Si | 5690.4250 | 2.05 | 3.61 | 1770 | 0.220 | b |
| 14 | Si | 5701.1040 | 2.05 | 3.60 | 1770 | 0.220 | b |
| 14 | Si | 5793.0730 | 2.05 | 3.54 | 1700 | 0.230 | b |
| 20 | Ca | 5512.9800 | 2.07 | 3.83 | c | ||
| 20 | Ca | 5867.5620 | 2.07 | 3.57 | d | ||
| 21 | Sc | 5356.0910 | 1.603 | 2.137 | 412 | 0.271 | |
| 21 | Sc | 5484.6260 | 1.601 | 2.113 | 401 | 0.281 | |
| 24 | Cr | 5788.3820 | 1.408 | 1.953 | 316 | 0.264 | |
| 26 | Fe | 4962.5719 | 1.854 | 3.052 | 905 | 0.278 | |
| 26 | Fe | 4802.8797 | 1.794 | 1.862 | 356 | 0.244 | |
| 26 | Fe | 4985.2529 | 1.857 | 2.360 | 742 | 0.240 | |
| 26 | Fe | 5060.0780 | 1.312 | 1.579 | 205 | 0.252 | |
| 26 | Fe | 5293.9588 | 1.846 | 1.918 | 290 | 0.250 | b |
| 26 | Fe | 5365.3990 | 1.412 | 1.855 | 283 | 0.261 | |
| 26 | Fe | 5464.2796 | 1.846 | 1.900 | 380 | 0.250 | b |
| 26 | Fe | 5494.4626 | 1.830 | 1.644 | 330 | 0.290 | b |
| 26 | Fe | 5655.1760 | 2.189 | 4.583 | 2010 | 0.250 | b |
| 26 | Fe | 5662.5160 | 1.862 | 2.337 | 724 | 0.235 | |
| 26 | Fe | 5775.0806 | 1.872 | 2.337 | 720 | 0.231 | |
| 26 | Fe | 5853.1483 | 1.430 | 1.778 | 264 | 0.242 | |
| 26 | Fe | 6027.0509 | 1.830 | 1.908 | 380 | 0.250 | b |
| 26 | Fe | 6120.2460 | 1.376 | 1.661 | 229 | 0.252 | e |
| 26 | Fe | 6127.9060 | 1.846 | 1.917 | 290 | 0.250 | b |
| 26 | Fe | 6157.7279 | 1.830 | 1.897 | 375 | 0.255 | b |
| 26 | Fe | 6165.3600 | 1.846 | 1.914 | 380 | 0.250 | b |
| 26 | Fe | 6301.5000 | 1.789 | 2.441 | 832 | 0.243 | |
| 26 | Fe | 6315.8110 | 1.830 | 1.682 | 410 | 0.250 | b |
| 26 | Fe | 6380.7430 | 1.856 | 1.907 | 380 | 0.250 | b |
| 26 | Fe | 6400.3170 | 1.376 | 1.646 | 226 | 0.253 | |
| 26 | Fe | 6574.2270 | 1.380 | 1.645 | 227 | 0.254 | |
| 26 | Fe | 6648.0800 | 1.385 | 1.650 | 229 | 0.254 | e |
| 26 | Fe | 8515.1084 | 1.674 | 1.936 | 356 | 0.242 | |
| 26 | Fe | 8582.2574 | 1.669 | 1.925 | 352 | 0.244 | |
| 26 | Fe | 8621.6007 | 1.662 | 1.913 | 347 | 0.246 | |
| 26 | Fe | 8699.4540 | 2.148 | 2.989 | 817 | 0.272 | |
| 26 | Fe | 8922.6500 | 2.173 | 3.022 | 839 | 0.278 | |
| 30 | Zn | 4810.5280 | 1.599 | 2.228 | 676 | 0.238 | |
| 40 | Zr | 6127.4750 | 1.449 | 1.747 | 260 | 0.244 | |
| 40 | Zr | 6134.5850 | 1.432 | 1.717 | 251 | 0.248 | |
| 40 | Zr | 6140.5350 | 1.491 | 1.822 | 287 | 0.242 | |
| 42 | Mo | 6030.6440 | 1.392 | 1.969 | 322 | 0.262 |
Notes. ABO theory broadening data are given as cross section σ in atomic units and velocity exponent α. Broadening data were either interpolated in the tables of Anstee & O’Mara (1995) and Barklem & O’Mara (1997) or calculated by PSB. (a) p–p transition; s–p table was used; loggf = − 8. (b) New calculation or estimate by PSB. (c) p–p transition; outside range of s–p table. (d) σ = 2170 a.u. at v = 104 m s−1; α could not be determined because of poor dependence of σ on v. (e) log gf < −5.
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