Table 3
Temperatures and surface gravities for stars redder than the u-jump that do not show evidence of radiative levitation as derived from the a0 and sz parameters and from line profile fits for an assumed metallicity of [M/H] = −1.5.
ID | Photometric parameters | Spectroscopic parameters | |||||
a 0 | sz | T eff | log g | T eff | log g |
![]() |
|
[mmag] | [mmag] | [K] | [K] | ||||
|
|||||||
52 | +48 ± 4 | 91 ± 5 | 9100 ± 380 | 3.39 ± 0.11 | 8240 ± 20 | 2.87 ± 0.02 | |
55 | +124 ± 4 | 91 ± 4 | 8100 ± 260 | 3.08 ± 0.15 | |||
60 | +134 ± 6 | 89 ± 7 | 8000 ± 260 | 3.05 ± 0.19 | |||
61 | +151 ± 3 | 79 ± 3 | 7900 ± 210 | 3.09 ± 0.16 | |||
63 | +125 ± 5 | 95 ± 5 | 8100 ± 270 | 3.02 ± 0.17 | |||
70 | +82 ± 4 | 86 ± 4 | 8600 ± 330 | 3.36 ± 0.12 | 7990 ± 20 | 2.94 ± 0.03 | |
72 | +114 ± 7 | 86 ± 8 | 8200 ± 300 | 3.21 ± 0.18 | |||
74 | +81 ± 3 | 85 ± 3 | 8600 ± 320 | 3.37 ± 0.11 | 7910 ± 10 | 2.94 ± 0.04 | |
79 | +79 ± 5 | 86 ± 5 | 8600 ± 340 | 3.37 ± 0.13 | 7990 ± 10 | 2.97 ± 0.03 | |
81 | +54 ± 3 | 84 ± 3 | 9000 ± 350 | 3.47 ± 0.10 | 8210 ± 20 | 2.98 ± 0.02 | |
83 | +34 ± 4 | 80 ± 4 | 9300 ± 400 | 3.57 ± 0.10 | 8360 ± 30 | 3.02 ± 0.02 | |
86 | +57 ± 3 | 84 ± 4 | 8900 ± 360 | 3.46 ± 0.10 | 8160 ± 20 | 3.00 ± 0.02 | |
88 | +30 ± 5 | 88 ± 6 | 9300 ± 420 | 3.46 ± 0.11 | 8390 ± 30 | 2.98 ± 0.02 | |
89 | +56 ± 3 | 81 ± 3 | 8900 ± 360 | 3.51 ± 0.10 | 8070 ± 20 | 2.93 ± 0.03 | |
90 | +27 ± 7 | 87 ± 10 | 9400 ± 470 | 3.48 ± 0.14 | 8450 ± 30 | 3.04 ± 0.02 | |
96 | +5 ± 7 | 84 ± 7 | 9700 ± 500 | 3.54 ± 0.12 | 8560 ± 30 | 3.07 ± 0.02 | |
99 | −17 ± 6 | 80 ± 7 | 10 100 ± 510 | 3.61 ± 0.12 | 9130 ± 260 | 3.25 ± 0.15 | −0.6 |
102 | 0 ± 3 | 86 ± 3 | 9800 ± 440 | 3.51 ± 0.09 | 9290 ± 320 | 3.38 ± 0.18 | −1.4 |
103 | −56 ± 6 | 86 ± 7 | 10 900 ± 590 | 3.42 ± 0.19 | 9850 ± 70 | 3.34 ± 0.04 | −1.0 |
106 | −8 ± 5 | 84 ± 6 | 10 000 ± 490 | 3.54 ± 0.11 | 9230 ± 290 | 3.33 ± 0.17 | −1.3 |
107 | −5 ± 4 | 85 ± 4 | 9900 ± 460 | 3.52 ± 0.10 | 9350 ± 260 | 3.39 ± 0.15 | −1.2 |
111 | −52 ± 6 | 68 ± 6 | 10 800 ± 570 | 3.82 ± 0.12 | 9760 ± 90 | 3.44 ± 0.05 | −1.0 |
113 | −17 ± 3 | 85 ± 4 | 10 100 ± 470 | 3.52 ± 0.11 | 9210 ± 180 | 3.31 ± 0.11 | −0.8 |
114 | −27 ± 9 | 81 ± 11 | 10 300 ± 600 | 3.58 ± 0.17 | 9340 ± 140 | 3.33 ± 0.08 | −1.0 |
115 | −16 ± 4 | 86 ± 5 | 10 100 ± 480 | 3.50 ± 0.12 | 9280 ± 180 | 3.34 ± 0.10 | −1.1 |
118 | −27 ± 3 | 86 ± 3 | 10 300 ± 480 | 3.49 ± 0.11 | 9440 ± 90 | 3.38 ± 0.05 | −1.1 |
119 | −16 ± 3 | 87 ± 4 | 10 100 ± 470 | 3.48 ± 0.11 | 9430 ± 170 | 3.39 ± 0.09 | −1.2 |
120 | −32 ± 9 | 80 ± 10 | 10 400 ± 600 | 3.60 ± 0.17 | 9470 ± 70 | 3.39 ± 0.04 | −1.0 |
122 | −47 ± 7 | 77 ± 9 | 10 700 ± 590 | 3.64 ± 0.17 | 9740 ± 80 | 3.40 ± 0.04 | −1.1 |
127 | −63 ± 4 | 89 ± 4 | 11 000 ± 550 | 3.33 ± 0.18 | 9920 ± 80 | 3.37 ± 0.04 | −0.8 |
143 | −42 ± 5 | 84 ± 6 | 10 600 ± 550 | 3.50 ± 0.16 | 9810 ± 60 | 3.45 ± 0.03 | −1.1 |
145 | −46 ± 3 | 82 ± 3 | 10 700 ± 520 | 3.54 ± 0.12 | 9660 ± 60 | 3.42 ± 0.03 | −1.0 |
147 | −54 ± 4 | 73 ± 5 | 10 800 ± 550 | 3.71 ± 0.12 | 9810 ± 80 | 3.43 ± 0.04 | −0.8 |
149 | −67 ± 5 | 78 ± 5 | 11 100 ± 590 | 3.58 ± 0.17 | 9800 ± 80 | 3.41 ± 0.04 | −1.0 |
151 | −53 ± 4 | 72 ± 4 | 10 800 ± 540 | 3.74 ± 0.11 | 9760 ± 80 | 3.43 ± 0.04 | −0.9 |
154 | −51 ± 3 | 88 ± 4 | 10 800 ± 520 | 3.39 ± 0.15 | 10 100 ± 100 | 3.51 ± 0.04 | −1.1 |
156 | −46 ± 8 | 88 ± 10 | 10 700 ± 610 | 3.40 ± 0.22 | 9760 ± 80 | 3.37 ± 0.04 | −1.0 |
157 | −52 ± 11 | 79 ± 13 | 10 800 ± 670 | 3.59 ± 0.23 | 9580 ± 90 | 3.34 ± 0.05 | −1.1 |
169 | −88 ± 4 | 72 ± 5 | 11 600 ± 600 | 3.69 ± 0.17 | 10 400 ± 100 | 3.53 ± 0.05 | −1.0 |
176 | −72 ± 5 | 80 ± 6 | 11 200 ± 600 | 3.52 ± 0.19 | 10 300 ± 100 | 3.52 ± 0.05 | −1.0 |
180 | −75 ± 4 | 82 ± 5 | 11 300 ± 580 | 3.46 ± 0.18 | 10 600 ± 80 | 3.60 ± 0.04 | −1.1 |
Notes. The errors for the photometric results are derived from the
errors of a0 and sz in combination
with the errors of the fits and an uncertainty of
002 for
the reddening (see Sect. 5.1 for details). The
errors for the spectroscopic results are derived from the χ2 fit
(see Sect. 5.2 for details) and are only
statistical errors. In addition, we list the helium abundance as determined with
LINFOR (see Sect. 6 for details).
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