Colour |
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Colour range | a0 | a1 | a2 | a3 | a4 | a5 | N |
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B-V | [-5.0,0.4] | [0.18,1.29] | 0.5665 | 0.4809 | -0.0060 | -0.0613 | -0.0042 | -0.0055 | 400 | 73 |
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[-5.0,0.3] | [0.24,0.80] | 0.4386 | 1.4614 | -0.7014 | -0.0807 | 0.0142 | -0.0015 | 201 | 62 |
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[-5.0,0.3] | [0.23,0.68] | 0.3296 | 1.9716 | -1.0225 | -0.0298 | 0.0329 | 0.0035 | 211 | 82 |
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[-5.0,0.3] | [0.46,1.47] | 0.4033 | 0.8171 | -0.1987 | -0.0409 | 0.0319 | 0.0012 | 208 | 59 |
V-J | [-5.0,0.4] | [0.61,2.44] | 0.4669 | 0.3849 | -0.0350 | -0.0140 | 0.0225 | 0.0011 | 401 | 42 |
V-H | [-5.0,0.4] | [0.67,3.01] | 0.5251 | 0.2553 | -0.0119 | -0.0187 | 0.0410 | 0.0025 | 401 | 33 |
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[-5.0,0.4] | [0.78,3.15] | 0.5057 | 0.2600 | -0.0146 | -0.0131 | 0.0288 | 0.0016 | 401 | 25 |
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[-5.0,0.4] | [0.07,0.80] | 0.6393 | 0.6104 | 0.0920 | -0.0330 | 0.0291 | 0.0020 | 412 | 132 |
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[-2.7,0.4] | [0.19,1.49] | 0.5839 | 0.4000 | -0.0067 | -0.0282 | -0.0346 | -0.0087 | 251 | 79 |
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[-2.7,0.4] | [0.77,2.56] | 0.4525 | 0.3797 | -0.0357 | -0.0082 | 0.0123 | -0.0009 | 272 | 43 |
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[-2.7,0.4] | [0.77,3.16] | 0.5286 | 0.2354 | -0.0073 | -0.0182 | 0.0401 | 0.0021 | 263 | 26 |
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[-2.4,0.4] | [0.99,3.29] | 0.4892 | 0.2634 | -0.0165 | -0.0121 | 0.0249 | -0.0001 | 258 | 18 |
b-y | [-3.7,0.5] | [0.18,0.72] | 0.5796 | 0.4812 | 0.5747 | -0.0633 | 0.0042 | -0.0055 | 1120 | 62 |
Notes. The photometric systems are Johnson-Cousins
,
2MASS
,
Tycho2
and Strömgren by. For the latter, additional corrections as
function of
and (b-y) apply, as discussed in Sect. 6.1.1.
For some indices the calibrations are given down to
,
meaning that
the effective temperatures of such a metal-poor star can be recovered using
in Eq. (3). Notice that only two hyper metal-poor stars
are currently known and caution should be used, as discussed in the text.
Especially for metal-poor stars, please refer to Fig. 13 to check
that the calibration is not extrapolated outside its
range.
N is the number of stars employed for the fit after the
clipping and
is the standard deviation (in Kelvin) of the
proposed calibrations. Notice that the standard deviation does not account for
the uncertainty in the zero point of the temperature scale, which is of order
15-20 K (Sects. 3.2 and 4.1).
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