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Table 4:

Coefficients and range of applicability of the colour-temperature-metallicity relations.

Colour
${\rm [Fe/H]}$ range Colour range a0 a1 a2 a3 a4 a5 N $\sigma (T_{\rm eff})$
B-V [-5.0,0.4] [0.18,1.29] 0.5665 0.4809 -0.0060 -0.0613 -0.0042 -0.0055 400 73
$V-R_{\rm C}$ [-5.0,0.3] [0.24,0.80] 0.4386 1.4614 -0.7014 -0.0807 0.0142 -0.0015 201 62
$(R-I)_{\rm C}$ [-5.0,0.3] [0.23,0.68] 0.3296 1.9716 -1.0225 -0.0298 0.0329 0.0035 211 82
$V-I_{\rm C}$ [-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
$V-K_{\rm S}$ [-5.0,0.4] [0.78,3.15] 0.5057 0.2600 -0.0146 -0.0131 0.0288 0.0016 401 25
$J-K_{\rm S}$ [-5.0,0.4] [0.07,0.80] 0.6393 0.6104 0.0920 -0.0330 0.0291 0.0020 412 132
$(B-V)_{\rm T}$ [-2.7,0.4] [0.19,1.49] 0.5839 0.4000 -0.0067 -0.0282 -0.0346 -0.0087 251 79
$V_{\rm T}-J$ [-2.7,0.4] [0.77,2.56] 0.4525 0.3797 -0.0357 -0.0082 0.0123 -0.0009 272 43
$V_{\rm T}-H$ [-2.7,0.4] [0.77,3.16] 0.5286 0.2354 -0.0073 -0.0182 0.0401 0.0021 263 26
$V_{\rm T}-K_{\rm S}$ [-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 $BV(RI)_{\rm C}$, 2MASS $JHK_{\rm S}$, Tycho2 $(BV)_{\rm T}$ and Strömgren by. For the latter, additional corrections as function of ${\rm [Fe/H]}$ and (b-y) apply, as discussed in Sect. 6.1.1. For some indices the calibrations are given down to ${\rm [Fe/H]}=-5.0$, meaning that the effective temperatures of such a metal-poor star can be recovered using ${\rm [Fe/H]}= -3.5$ 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 ${\rm [Fe/H]}$ range. N is the number of stars employed for the fit after the $3 \sigma$clipping and $\sigma (T_{\rm eff})$ 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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