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Table 1:

Far-UV and IR fractions of the unobserved bolometric flux as a function of $T_{\rm eff}$ and $\log g$, the function  $\Lambda(T_{\rm eff},\log g)$, and temperatures  $T_{\rm eff}^f$ as a function of  $T_{\rm eff}(\gamma )$.
  $\log g = 4.0$ $\log g = 3.0$ $\log g = 2.5$
$T_{\rm eff}(\gamma )$ $\delta^*_{\rm UV}$ $\delta^*_{\rm IR}$ $\Lambda[T_{\rm eff}(\gamma),g]$ $\gamma $ $T_{\rm eff}^f$ $\delta^*_{\rm UV}$ $\delta^*_{\rm IR}$ $\Lambda[T_{\rm eff}(\gamma),g]$ $\gamma $ $T_{\rm eff}^f$ $\delta^*_{\rm UV}$ $\delta^*_{\rm IR}$ $\Lambda[T_{\rm eff}(\gamma),g]$ $\gamma $ $T_{\rm eff}^f$
10 000 0.023 0.059 0.024 1.5 9970 0.024 0.059 0.028 1.5 9970 0.023 0.059 0.029 1.5 9960
        2.0 9940       2.0 9930       2.0 9930
12 500 0.105 0.034 0.088 1.5 12 360 0.099 0.034 0.086 1.5 12 360 0.093 0.034 0.081 1.5 12 370
        2.0 12 220       2.0 12 220       2.0 12 240
15 000 0.230 0.022 0.152 1.5 14 710 0.218 0.022 0.135 1.5 14 740 0.202 0.022 0.122 1.5 14 770
        2.0 14 390       2.0 14 470       2.0 14 520
17 500 0.386 0.016 0.182 1.5 17 090 0.353 0.016 0.155 1.5 17 150 0.318 0.016 0.134 1.5 17 200
        2.0 16 640       2.0 16 780       2.0 16 880
20 000 0.552 0.012 0.194 1.5 19 450 0.484 0.012 0.157 1.5 19 600 0.450 0.012 0.135 1.5 19 650
        2.0 18 950       2.0 19 160       2.0 19 290
22 500 0.706 0.009 0.191 1.5 21 940 0.596 0.010 0.139 1.5 22 090 0.546 0.010 0.109 1.5 22 190
        2.0 21 340       2.0 21 670       2.0 21 860
25 000 0.843 0.008 0.178 1.5 24 420 0.693 0.008 0.106 1.5 24 670 0.635 0.008 0.071 1.5 24 780
        2.0 23 800       2.0 24 310       2.0 24 540
27 500 0.955 0.007 0.153 1.5 26 950 0.823 0.007 0.093 1.5 27 180          
        2.0 26 380       2.0 26 840          
30 000 1.060 0.006 0.126 1.5 29 520 1.023 0.006 0.087 1.5 29 670          
        2.0 29 010       2.0 29 330          
32 500 1.241 0.005 0.109 1.5 32 050                    
        2.0 31 580                    
35 000 1.539 0.004 0.103 1.5 34 540                    
        2.0 34 060                    
For $\Lambda(T_{\rm eff})$ and $T_{\rm eff}$ the temperature $T_{\rm eff}(\gamma )$ is simply the effective temperature written in the first column of the table.
Parameters $\delta^*_{\rm UV}$ and $\delta^*_{\rm IR}$ are values of $\delta_{\rm UV}$ and $\delta_{\rm IR}$ calculated with $T_{\rm eff}(\gamma )$ and fluxes $F_{\lambda}[T_{\rm eff}(\gamma),\log g]$, which do not undergo the transformation given by Eq. (6). To calculate them we have used $\lambda_a=1380$ Å and $\lambda_b=11~084$ Å. Note that $T^f_{\rm eff}=$ $T_{\rm eff}(\gamma=1)$.

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