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MA![]() |
MA![]() |
Classical, EW | ||||||||
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[Fe/H] |
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[Fe/H] |
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[Fe/H] | vt (km s-1) |
HD 3567 | 6103.5 | 4.79 | -1.200 | 6176.0 | 4.20 | -1.223 | 6035.0 | 4.08 | -1.200 | 1.50 |
HD 19445 | - | - | - | 5746.5 | 4.10 | -2.293 | 5982.0 | 4.38 | -2.075 | 1.40 |
HD 22879 | 5770.6 | 4.31 | -0.877 | 5778.1 | 4.31 | -0.880 | 5792.0 | 4.29 | -0.885 | 1.20 |
HD 25704 | 5638.9 | 3.61 | -1.094 | 5864.4 | 4.19 | -0.912 | 5700.0 | 4.18 | -1.010 | 1.00 |
HD 63077 | 5795.5 | 4.21 | -0.796 | 5787.7 | 4.21 | -0.793 | 5629.0 | 4.15 | -0.935 | 0.90 |
HD 63598 | 6078.6 | 4.79 | -0.681 | 5804.1 | 4.23 | -0.901 | 5680.0 | 4.16 | -0.885 | 0.90 |
HD 97320 | 5601.1 | 4.65 | -1.411 | 6025.1 | 4.24 | -1.183 | 6105.0 | 4.18 | -1.175 | 1.20 |
HD 103723 | 5999.2 | 4.29 | -0.896 | 6004.4 | 4.29 | -0.896 | 6128.0 | 4.28 | -0.805 | 1.50 |
HD 105004 | 5802.5 | 4.33 | -0.900 | 5802.5 | 4.33 | -0.900 | 5900.0 | 4.30 | -0.800 | 1.10 |
HD 106038 | 5994.6 | 4.48 | -1.392 | 5995.5 | 4.48 | -1.392 | 5950.0 | 4.33 | -1.390 | 1.10 |
HD 113679 | 6037.3 | 4.73 | -0.500 | 5757.5 | 4.35 | -0.708 | 5759.0 | 4.04 | -0.590 | 0.90 |
HD 116064 | 5757.7 | 4.58 | -2.41 | 5757.7 | 4.58 | -2.401 | 5999.0 | 4.33 | -2.000 | 1.50 |
HD 121004 | 5509.2 | 4.05 | -0.670 | 5657.8 | 4.40 | -0.650 | 5711.0 | 4.46 | -0.725 | 0.65 |
HD 122196 | 5811.8 | 3.50 | -1.954 | 5810.2 | 3.56 | -1.954 | 6048.0 | 3.89 | -1.760 | 1.20 |
HD 126681 | 5556.9 | 4.44 | -1.055 | 5521.6 | 4.68 | -1.075 | 5532.0 | 4.58 | -1.170 | 0.60 |
HD 160617 | 5804.1 | 3.50 | -1.961 | 5985.2 | 3.75 | -1.794 | 6028.0 | 3.79 | -1.785 | 1.30 |
HD 175179 | 6080.5 | 5.00 | -0.500 | 5779.5 | 4.47 | -0.691 | 5758.0 | 4.16 | -0.690 | 0.90 |
HD 188510 | 5568.8 | 4.35 | -1.341 | 5500.0 | 4.65 | -1.231 | 5536.0 | 4.63 | -1.600 | 1.00 |
HD 189558 | 5610.8 | 3.58 | -1.191 | 5500.0 | 3.75 | -1.181 | 5712.0 | 3.79 | -1.145 | 1.20 |
HD 195633 | 6318.2 | 4.61 | -0.500 | 6037.7 | 3.99 | -0.687 | 6005.0 | 3.86 | -0.625 | 1.40 |
HD 205650 | 5693.7 | 4.93 | -1.195 | 5754.0 | 4.47 | -1.208 | 5842.0 | 4.49 | -1.170 | 0.90 |
HD 298986 | 5891.5 | 3.66 | -1.592 | 6297.9 | 4.22 | -1.304 | 6144.0 | 4.18 | -1.410 | 1.40 |
CD-333337 | 5808.2 | 3.66 | -1.598 | 5946.9 | 3.85 | -1.490 | 5952.0 | 3.95 | -1.435 | 1.40 |
CD-453283 | 5500.0 | 4.26 | -0.978 | 5885.5 | 5.00 | -0.685 | 5657.0 | 4.97 | -0.835 | 0.80 |
CD-571633 | 5939.9 | 4.37 | -0.893 | 5939.9 | 4.37 | -0.893 | 5907.0 | 4.26 | -0.930 | 1.10 |
CD-3018140 | 6143.1 | 3.50 | -2.095 | 6246.5 | 3.50 | -1.980 | 6340.0 | 4.13 | -1.870 | 1.00 |
G005-040 | 6228.2 | 5.00 | -0.584 | 5930.4 | 4.52 | -0.794 | 5766.0 | 4.23 | -0.840 | 0.80 |
G013-009 | 6529.5 | 4.58 | -2.29 | 6556.0 | 4.08 | -2.299 | 6416.0 | 3.95 | -2.225 | 1.40 |
Notes. In
the first analysis all three parameters are determined with only the
spectrum, while in the second one
was determined independently by using parallaxes according to
Eq. (14), as for the classical method (EW; last four columns).
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