Table 1: Set of visible and infrared lines considered in this work. $\lambda _{0}$ represents the central wavelength, $\chi $ the excitation potential of the lower level, $\log ~ gf$ the logarithm of the oscillator strength times the multiplicity of the lower level, and $g_{\rm eff}$ the effective Landé factor.
Species $\lambda _{0}$ [nm] $\chi $ [eV] $\log{ gf}$ $g_{\rm eff}$
Ni I 491.20 3.75 -0.87 0.00
Fe I 524.71 0.09 -4.95 2.00
Fe I 525.02 0.12 -4.94 3.00
Fe I 537.96 3.69 -1.65 1.00
Ti II 538.10 1.57 -2.05 0.90
Fe I 557.61 3.43 -0.91 0.00
Fe I 569.15 4.30 -1.36 0.00
Fe II 614.93 3.89 -2.70 1.33
Fe I 617.33 2.22 -2.98 2.50
Fe I 630.25 3.69 -1.24 2.50
Fe I 630.35 4.32 -2.55 1.50
Ti I 630.38 1.45 -1.44 0.92
Ni I 676.78 1.83 -1.89 1.50
Fe I 709.04 4.23 -1.21 0.00
Fe II 722.45 3.89 -3.39 0.00
Si I 1062.76 5.86 -0.29 1.75
Fe I 1089.63 3.07 -2.85 1.50
Fe I 1142.23 2.20 -2.89 1.98
Fe I 1221.33 4.64 -1.93 2.50
Fe I 1558.83 6.37 +0.25 1.50
Fe I 1564.85 5.43 -0.67 3.00


Source LaTeX | All tables | In the text