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Table A.1:

Fe I and FeII line list, wavelength, excitation potential, damping constant, gf-values and equivalent widths.
Species ${\rm\lambda}$ ${\rm\chi_{ex}}$ ${\rm C_6}$ log gf log gf B-8 B-107 B-108 B-118 B-122 B-128 B-130 B-134 F-121
  ( Å) (eV) ${\rm cm^6~s^{-1}}$ FW06 present                  
FeII 6149.26 3.89 0.34E-32 -2.84 -2.69 18 31 22 23 25 31 32 40 20
FeII 6247.56 3.89 0.33E-32 -2.43 -1.98 43 51 25 43 42 44 43 57 43
FeII 6432.68 2.89 0.24E-32 -3.57 -3.57 35 42 28 29 33 38 38 38 30
FeII 6456.39 3.90 0.32E-32 -2.19 -2.05 60 76 49 62 53 51 53 85 47
FeII 6516.08 2.89 0.25E-32 -3.37 -3.31 52 53 34 40 44 44 43 60 49
FeI 6151.62 2.18 0.81E-32 same -3.299 73 44 52 74 59 68 52 27 56
FeI 6159.38 4.61 0.13E-30 absent -1.97 24 - - - - - 13 - -
FeI 6165.36 4.14 0.77E-31 -1.474 -1.549 32 23 - 37 - 29 25 7 25
FeI 6173.34 2.22 0.84E-32 -2.880 -2.879 95 67 62 99 88 92 78 - 75
FeI 6180.20 2.73 0.13E-31 -2.650 -2.784 78 44 50 68 58 70 60 12 54
FeI 6187.99 3.94 0.30E-30 -1.670 -1.718 40 22 21 42 27 34 31 19 26
FeI 6200.31 2.61 0.15E-31 same -2.437 83 64 66 81 73 81 76 11 75
FeI 6213.43 2.22 0.30E-31 -2.48 -2.646 109 87 78 99 96 98 91 35 87
FeI 6220.78 3.88 0.13E-30 absent -2.46 22 11 - 16 - - - - 12
FeI 6226.74 3.88 0.13E-30 absent -2.202 23 16 - 15 16 17 15 17 17
FeI 6240.65 2.22 0.10E-31 -3.17 -3.388 71 86 45 68 57 73 50 - 56
FeI 6246.32 3.60 0.12E-30 -0.877 -0.956 102 86 73 102 95 110 100 64 99
FeI 6252.56 2.40 0.12E-31 same -1.687 140 117 103 126 116 118 119 82 119
FeI 6254.25 2.28 0.13E-31 -2.426 -2.480 115 103 87 127 108 116 106 52 106
FeI 6270.23 2.86 0.15E-31 -2.61 -2.711 73 36 51 67 60 72 62 21 56
FeI 6271.28 3.32 0.89E-31 -2.703 -2.957 17 9 18 21 - 12 - 13 14
FeI 6297.79 2.22 0.82E-32 same -2.740 97 58 63 88 75 90 72 25 71
FeI 6301.50 3.65 0.23E-31 -0.718 -0.720 100 90 67 89 84 86 90 - 86
FeI 6302.50 3.69 0.23E-31 absent -0.91 91 75 66 70 72 88 79 37 73
FeI 6311.50 2.83 0.14E-31 -3.141 -3.224 46 28 38 45 43 46 44 32 25
FeI 6315.31 4.14 0.30E-31 -1.232 -1.230 55 42 33 52 42 48 33 - 43
FeI 6315.81 4.08 0.66E-31 -1.660 -1.712 38 30 30 41 42 39 30 - 23
FeI 6322.69 2.59 0.14E-31 same -2.426 92 69 59 91 77 89 70 28 78
FeI 6335.33 2.20 0.80E-32 -2.177 -2.229 114 106 90 109 110 120 103 - 99
FeI 6336.82 3.69 0.13E-30 -0.856 -1.053 101 77 70 90 80 - 69 36 84
FeI 6344.15 2.43 0.12E-31 -2.923 -2.922 93 56 55 78 75 84 65 29 70
FeI 6355.03 2.84 0.30E-31 -2.291 -2.40 97 35 58 89 80 94 70 24 74
FeI 6392.54 2.28 0.11E-31 absent -4.03 42 - - 31 18 24 31 - 21
FeI 6393.60 2.43 0.12E-31 -1.58 -1.615 183 136 107 144 123 152 143 - 107
FeI 6419.95 4.73 0.15E-30 -0.27 -0.250 64 41 47 66 53 62 53 28 52
FeI 6430.85 2.18 0.77E-32 -2.006 -2.005 133 112 116 133 121 133 124 74 97
FeI 6475.62 2.56 0.15E-31 same -2.94 77 42 57 77 57 64 61 17 44
FeI 6481.87 2.28 0.11E-31 same -2.984 87 58 64 81 72 78 74 25 55
FeI 6498.94 0.96 0.49E-32 -4.687 -4.699 87 44 74 71 68 73 70 15 51
FeI 6518.37 2.83 0.13E-31 -2.30 -2.748 61 46 45 50 60 61 48 19 50
FeI 6533.93 4.56 0.16E-30 -1.43 -1.453 20 19 - - 25 - 25 - 19
FeI 6569.22 4.73 0.13E-30 -0.45 -0.422 59 38 49 62 52 69 62 - 45
FeI 6574.23 0.99 0.56E-32 -5.004 -5.042 63 18 41 64 49 50 45 - 51
FeI 6575.02 2.59 0.14E-31 -2.71 -2.824 85 47 57 78 69 79 64 - 62
FeI 6591.31 4.59 0.12E-30 absent -2.06 - - - - - 9 - - -
FeI 6593.87 2.43 0.12E-31 same -2.422 105 86 86 115 98 105 87 - 80
FeI 6597.56 4.80 0.15E-30 -1.05 -1.061 33 13 21 28 31 34 17 19 25
FeI 6608.03 2.28 0.10E-31 absent -4.038 16 7 - 14 25 15 13 6 16
FeI 6678.00 2.69 0.30E-31 absent -1.420 147 118 - 150 139 148 134 - 128
FeI 6703.57 2.76 0.12E-31 -3.06 -3.15 51 35 28 40 37 54 19 19 33
FeI 6705.11 4.61 0.30E-31 absent -1.060 34 - - 29 12 40 26 - 22
FeI 6710.32 1.48 0.64E-32 absent -4.874 46 14 - 49 31 46 32 - 34
FeI 6713.75 4.80 0.16E-30 absent -1.602 - - - 16 - - 5 - 7
FeI 6715.38 4.59 0.11E-30 absent -1.638 32 17 - 14 12 27 18 - 18
FeI 6716.24 4.56 0.79E-32 absent -1.927 15 11 - - 8 31 10 - 11
FeI 6725.36 4.10 0.15E-30 absent -2.300 - - - 9 10 5 20 - 16
FeI 6726.67 4.59 0.30E-31 absent -1.090 22 - 27 24 34 18 32 - 24
FeI 6733.15 4.64 0.11E-30 absent -1.576 25 22 - 30 27 31 18 - 23
FeI 6739.52 1.56 0.67E-32 -4.79 -4.941 33 - - 26 36 25 25 - 30
FeI 6752.71 4.64 0.11E-30 -1.204 -1.366 22 27 - 23 28 23 6 - 21
FeI 6810.26 4.60 0.14E-30 -0.986 -1.108 31 11 - 44 25 35 32 - 17
FeI 6820.37 4.64 0.16E-30 -1.29 -1.311 36 12 - 45 23 30 14 - 24
FeI 6837.02 4.59 0.78E-32 -1.687 -1.800 13 - - 22 - - 24 - 14
FeI 6839.83 2.56 0.13E-31 -3.35 -3.451 49 24 - 37 32 47 35 - 27
FeI 6841.34 4.61 0.10E-30 -0.78 -0.752 49 27 - 56 53 55 17 - 39
FeI 6842.69 4.64 0.15E-30 -1.29 -1.315 20 11 - 23 44 38 - - 13
FeI 6843.66 4.55 0.94E-31 -0.89 -0.928 50 23 - 47 53 64 32 - 42
FeI 6851.63 1.60 0.73E-32 absent -5.307 26 21 - 18 20 30 8 - -
FeI 6855.71 4.39 0.10E-30 absent -1.819 33 35 - 45 17 28 25 - 28
FeI 6857.25 4.08 0.53E-31 absent -2.156 15 17 - 14 13 24 8 - 21
FeI 6858.15 4.61 0.10E-30 -0.93 -1.055 39 30 - 30 35 41 13 - 24

The oscillator strengths used in this paper and in Barbuy et al. (2007) are given in Col. 6, and compared to those given in Fuhr & Wiese (2006) in Col. 5. Equivalent widths were measured using DAOSPEC. For B-108 and B-134 the lines were checked with IRAF, and only very clean lines were kept.

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