Table 5: List of lines used in the abundance analysis, with references to the oscillator strengths used. The columns Waals. , Stark. , and Rad.  list the van der Waals, Stark, and radiative damping data (for a description of the data sources, see Barklem et al. 2005, Sect. 3.2, paragraph 5). Rad. is the logarithm (base 10) of the FWHM given in $\rm rad~s^{-1}$. Non-zero values of Stark.  and negative values of Waals.  represent the logarithm of FWHM per unit pertuber number density at 10 000 K, given in $\rm rad~s^{-1}cm^{-3}$. Positive values of the van der Waals parameter correspond to the notation of Anstee & O'Mara (1995), where a packed parameter is used for the broadening cross-section ($\sigma $) for collisions by neutral hydrogen at 10 km s-1 and its velocity dependence ($\alpha $). E.g. for the Mg I 5172.684 Å line, Waals. =729.238 means $\sigma =729$ in atomic units and  $\alpha =0.238$. d $\lambda _{\rm blue}$ and d $\lambda _{\rm red}$ give the extent of the spectral windows used for fitting of each line, blue-wards and red-wards of the central wavelength. Zero values in both columns indicate that the line-contribution is considered in the same window as the one listed directly above.
Ion $\lambda$ [Å] $\chi$ [eV] $\log{gf}$ Ref. Waals. Stark. Rad. d $\lambda _{\rm blue}$ [mÅ] d $\lambda _{\rm red}$ [mÅ]
Mg I 5172.684 2.712 -0.380 1 729.238 0. 7.990 -700 700
Mg I 5183.604 2.717 -0.160 1 729.238 0. 7.990 -700 700
Ca I 4434.957 1.886 -0.007 2 -7.162 -5.602 8.021 -300 100
Ca I 4435.679 1.886 -0.517 2 -7.163 -5.610 8.025 -300 300
Ca I 4454.779 1.899 0.258 2 -7.162 -5.596 8.017 -100 100
Ca I 4455.887 1.899 -0.518 2 -7.162 -5.602 8.021 -300 300
Ca I 5261.704 2.521 -0.579 3 -7.416 -5.756 7.903 -300 200
Ca I 5265.556 2.523 -0.113 3 -7.416 -5.755 7.903 -300 50
Ca I 6439.075 2.526 0.390 3 -7.704 -6.072 7.649 -300 300
Ca I 6462.567 2.523 0.262 3 -7.704 -6.072 7.645 -300 50
Ca I 6493.781 2.521 -0.109 3 -7.704 -6.071 7.640 -300 300
Ti I 4533.241 0.848 0.476 4 -7.593 -5.144 8.083 -300 300
Ti I 4534.776 0.836 0.280 4 -7.596 -5.313 8.079 -300 300
Ti I 4535.568 0.826 0.161 5 -7.840 -5.403 8.079 -300 50
Ti II 4394.059 1.221 -1.780 6 -7.944 -6.601 8.471 -100 300
Ti II 4395.840 1.243 -1.930 6 -7.904 -6.550 8.471 -200 200
Ti II 4399.765 1.237 -1.190 6 -7.946 -6.612 8.461 -300 200
Ti II 4417.714 1.165 -1.190 6 -7.926 -6.665 8.225 -300 300
Ti II 4443.801 1.080 -0.720 6 -7.923 -6.509 8.199 -200 300
Ti II 4450.482 1.084 -1.520 6 -7.920 -6.502 8.199 -300 200
Ti II 4468.507 1.131 -0.600 7 -7.931 -6.723 8.207 -300 300
Ti II 4470.853 1.165 -2.020 6 -7.928 -6.713 8.217 -250 150
Ti II 4501.270 1.116 -0.770 6 -7.931 -6.729 8.199 -300 300
Ti II 4533.960 1.237 -0.530 6 -7.960 -6.661 8.225 -300 100
Ti II 5185.902 1.893 -1.490 6 -7.908 -6.533 8.367 -300 300
Ti II 5226.538 1.566 -1.260 6 -7.953 -6.713 8.217 -300 70
Fe I 4375.930 0.000 -3.031 9 215.249 -6.320 4.622 -150 300
Fe I 4375.986 3.047 -2.029 8 -7.800 -5.760 7.810 0 0
Fe I 4383.545 1.485 0.208 9 295.265 -6.200 7.936 -300 300
Fe I 4404.750 1.557 -0.147 9 301.263 -6.200 7.969 -250 200
Fe I 4415.123 1.608 -0.621 9 308.257 -0.621 7.986 -150 200
Fe I 4427.310 0.052 -2.924 9 -7.880 -6.320 4.696 -100 300
Fe I 4430.614 2.223 -1.728 9 431.302 -6.080 8.606 -250 250
Fe I 4442.339 2.198 -1.228 9 424.302 -6.080 8.599 -300 300
Fe I 4443.194 2.858 -1.043 9 224.263 -6.340 7.799 -150 250
Fe I 4443.196 3.071 -1.905 8 -7.770 -6.020 8.010 0 0
Fe I 4447.717 2.223 -1.339 9 429.302 -6.080 8.604 -250 200
Fe I 4461.653 0.087 -3.210 7 -7.799 -6.320 4.638 -200 200
Fe I 4476.019 2.845 -0.819 9 -7.830 -6.170 7.825 -300 300
Fe I 4476.076 3.686 -0.175 8 -7.670 -4.730 7.935 0 0
Fe I 4482.170 0.110 -3.501 7 -7.799 -6.320 4.529 0 0
Fe I 4482.253 2.223 -1.482 9 -7.788 -6.080 8.599 0 0
Fe I 4489.739 0.121 -3.899 9 218.249 -6.320 4.403 -300 200
Fe I 4494.563 2.198 -1.143 9 416.302 -6.080 8.600 -300 300
Fe I 4528.614 2.176 -0.887 9 407.301 -6.080 8.607 -100 300
Fe I 4531.148 1.485 -2.155 7 -7.678 -6.200 8.083 -250 300
Fe I 4736.773 3.211 -0.752 9 820.231 -5.290 7.798 -200 200
Fe I 4871.318 2.865 -0.363 9 748.235 -5.490 8.005 -300 300
Fe I 4872.138 2.882 -0.567 9 754.235 -5.490 8.004 -300 300
Fe I 4890.755 2.875 -0.394 9 758.236 -5.240 8.004 -350 300
Fe I 4891.492 2.851 -0.112 9 750.237 -5.490 8.009 -300 350
Fe I 4903.310 2.882 -0.926 9 -7.259 -5.490 8.004 -300 300
Fe I 4918.994 2.865 -0.342 9 750.237 -5.490 8.009 -350 350
Fe I 4918.954 4.154 -0.635 8 -7.510 -4.690 8.470 0 0
Fe I 4920.503 2.832 0.068 9 739.238 -5.490 8.009 -300 300
Fe I 5150.840 0.990 -3.037 9 -7.742 -6.250 7.180 -300 300
Fe I 5166.282 0.000 -4.123 9 -7.826 -6.330 3.540 -180 180
Fe I 5171.596 1.485 -1.721 9 -7.687 -6.200 6.330 -220 220
Fe I 5191.455 3.038 -0.551 9 -7.258 -5.490 8.004 -300 300
Fe I 5192.344 2.998 -0.421 9 -7.266 -5.490 8.010 -300 250
Fe I 5194.942 1.557 -2.021 9 -7.680 -6.200 6.290 -300 200
Fe I 5202.336 2.176 -1.838 7 -7.603 -6.180 8.230 -300 300
Fe I 5202.256 4.256 -0.837 8 -7.765 -6.010 8.320 0 0
Fe I 5216.274 1.608 -2.082 9 -7.674 -6.200 6.220 -300 300
Fe I 5232.940 2.940 -0.058 9 -7.280 -5.490 8.009 -300 300
Fe I 5266.554 2.998 -0.386 9 -7.273 -5.489 8.009 -300 300
Fe I 5269.537 0.859 -1.321 7 -7.761 -6.300 7.185 -350 300
Fe I 5281.790 3.038 -0.834 9 -7.266 -5.490 8.010 -200 200
Fe I 5283.621 3.241 -0.524 9 -7.221 -5.450 7.880 -50 250
Fe I 5324.191 3.211 -0.103 10 -7.235 -5.500 7.880 -250 250
Fe I 5328.039 0.915 -1.466 7 -7.757 -6.302 7.161 -300 150
Fe I 5328.532 1.557 -1.850 9 -7.686 -6.228 6.848 -150 300
Fe I 5339.929 3.266 -0.647 10 -7.221 -5.451 7.874 -250 250
Fe I 6393.601 2.433 -1.576 9 -7.622 -6.310 7.970 -250 250
Fe I 6400.001 3.602 -0.290 10 -7.232 -5.500 7.900 -250 200
Fe I 6430.846 2.176 -1.946 9 -7.704 -6.190 8.220 -220 220
Fe I 6494.981 2.404 -1.273 7 -7.629 -6.330 7.936 -300 300
Fe II 4416.828 2.778 -2.540 11 -7.950 -6.670 8.614 -200 300
Fe II 4491.405 2.856 -2.700 12 -7.950 -6.600 8.481 -200 200
Fe II 4508.288 2.856 -2.312 13 -7.950 -6.670 8.617 -250 250
Fe II 4515.343 2.844 -2.362 14 -7.950 -6.600 8.487 -200 200
Fe II 4923.927 2.891 -1.206 14 -7.914 -6.583 8.489 -300 300
Fe II 5197.577 3.230 -2.100 12 -7.824 -6.600 8.480 -200 200
Fe II 5234.625 3.221 -2.270 15 -7.946 -6.600 8.490 -200 200
Fe II 5284.109 2.891 -3.130 11 -7.914 -6.600 8.530 -160 160
Fe II 5316.615 3.153 -1.850 12 -7.950 -6.600 8.480 -300 100
1 Wiese & Martin (1980); 2 Smith & O'Neill (1975); 3 Smith & Raggett (1981); 4 Blackwell et al. (1982); 5 R. Kurucz, http://cfaku5.cfa.harvard.edu/ATOMS/2200; 6 Pickering et al. (2001); 7 Martin et al. (1988); 8 R. Kurucz, http://cfaku5.cfa.harvard.edu/ATOMS/2600; 9 O'Brian et al. (1991); 10 Bard et al. (1991); 11 Moity (1983); 12 Kroll & Kock (1987); 13 Biemont et al. (1991); 14 Schnabel et al. (2004); 15 Heise & Kock (1990).


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