\begin{table}%T5
\par
\caption{\label{tab:cf}Coefficients and range of applicability of the flux
  calibrations for various $\phi_{\zeta} =
  \mathcal{F_{{\rm Bol}}}({\rm Earth})~10^{0.4~m_{\zeta}}$.}
  \small%\centering
\par
\begin{tabular}{llccccccccccc}
\hline\hline\noalign{\smallskip}
$\phi_{\zeta}$ & Colour & $\feh$ range & Colour range & $b_0$ & $b_1$ & $b_2$ & $b_3$ & $b_4$ & $b_5$ & $b_6$ & $N$ & $\sigma(\%)$ \\     
\noalign{\smallskip}\hline
$B_{\rm T}$ & $(B-V)_{\rm T}$ & $[-2.7,0.4]$ &  $[0.19,1.43]$ &   $2.1904$ &  $5.7106$   & $-6.7110$   & $7.4160$    & $-0.6704$   & $-0.1501$   & $-0.0720$   &  $260$  & $3.1$\\
$B_{\rm T}$ & $V_{\rm T}-J$   & $[-2.7,0.4]$ &  $[0.51,2.56]$ &   $1.8160$ &  $3.2833$   & $-2.3210$   & $1.7358$    & $1.2140$    & $-1.0830$   & $0.0343$    &  $261$  & $4.2$\\
$B_{\rm T}$ & $V_{\rm T}-H$   & $[-2.7,0.4]$ &  $[0.53,3.16]$ &   $1.7597$ &  $3.1896$   & $-1.8419$   & $0.9465$    & $0.9826$    & $-0.9055$   & $0.0809$    &  $255$  & $4.0$\\
$B_{\rm T}$ & $V_{\rm T}-K_{\rm S}$ & $[-2.7,0.4]$ &  $[0.59,3.29]$ &   $1.7202$ &  $3.0146$   & $-1.6377$   & $0.8033$    & $0.8591$    & $-0.8644$   & $0.0669$    &  $262$  & $3.9$\\
$V_{\rm T}$ & $(B-V)_{\rm T}$ & $[-2.7,0.4]$ &  $[0.19,1.43]$ &   $2.7098$ &  $-0.2765$  & $0.1523$    & $0.8122$    & $-0.2261$   & $-0.1789$   &  $-0.0413$  & $253$   & $2.7$\\
$V_{\rm T}$ & $V_{\rm T}-J$    & $[-2.7,0.4]$ &  $[0.62,2.53]$ &   $2.1815$ &  $0.9268$   & $-0.7701$   & $0.4029$    & $0.1047$    & $-0.2609$   &  $-0.0048$  & $249$   & $0.7$\\
$V_{\rm T}$ & $V_{\rm T}-H$    & $[-2.7,0.4]$ &  $[0.68,3.16]$ &   $2.1800$ &  $0.8514$   & $-0.5793$   & $0.2235$    & $0.0936$    & $-0.2458$   &  $0.0019$   & $261$   & $0.9$\\
$V_{\rm T}$ & $V_{\rm T}-K_{\rm S}$  & $[-2.7,0.4]$ &  $[0.59,3.29]$ &   $2.2565$ &  $0.6787$   & $-0.4536$   & $0.1800$    & $0.0785$    & $-0.2407$   &  $-0.0011$  & $256$   & $0.9$\\ 
$B$   & $B-V$     & $[-5.0,0.4]$ &  $[0.18,1.22]$ &   $1.9571$ &  $  6.9680$ & $ -11.0277$ & $  11.4450$ &   $-0.4975$ &   $-0.1276$ &   $-0.0432$ &   $331$ & $2.3$\\
$B$   & $V-R_{\rm C}$   & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.0002$ &  $  6.6483$ & $  -4.6407$ & $  25.3881$ &   $ 0.9547$ &   $-0.3756$ &   $-0.0067$ &   $186$ & $1.9$\\
$B$   & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.23,0.68]$ &   $9.8257$ &  $-57.0297$ & $ 152.2749$ & $ -77.6378$ &   $ 4.3253$ &   $-1.1377$ &   $ 0.0411$ &   $202$ & $3.2$\\
$B$   & $V-I_{\rm C}$   & $[-5.0,0.3]$ &  $[0.46,1.47]$ &   $4.3948$ &  $ -6.0713$ & $   9.6862$ & $   0.2327$ &   $ 0.9298$ &   $-0.5392$ &   $ 0.0089$ &   $196$ & $1.6$\\
$B$   & $V-J$     & $[-5.0,0.4]$ &  $[0.50,2.44]$ &   $1.6664$ &  $  3.5465$ & $  -2.5257$ & $   1.5310$ &   $ 0.4259$ &   $-0.4354$ &   $ 0.0047$ &   $332$ & $2.8$\\
$B$   & $V-H$     & $[-5.0,0.4]$ &  $[0.52,2.84]$ &   $1.6852$ &  $  3.2925$ & $  -1.9206$ & $   0.8026$ &   $ 0.2172$ &   $-0.1301$ &   $ 0.0346$ &   $328$ & $2.9$\\
$B$   & $V-K_{\rm S}$   & $[-5.0,0.4]$ &  $[0.57,3.03]$ &   $1.5185$ &  $  3.3566$ & $  -1.8830$ & $   0.7301$ &   $ 0.2887$ &   $-0.2929$ &   $ 0.0240$ &   $363$ & $2.8$\\
$V$   & $B-V$     & $[-5.0,0.4]$ &  $[0.30,1.03]$ &   $1.2581$ &  $  5.8828$ & $  -9.9287$ & $   6.8432$ &   $ 0.2290$ &   $-0.3935$ &   $-0.0420$ &   $241$ & $1.9$\\
$V$   & $V-R_{\rm C}$   & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.6659$ &  $ -1.6396$ & $   3.9243$ & $   2.9911$ &   $ 0.0978$ &   $-0.2339$ &   $-0.0252$ &   $177$ & $0.7$\\
$V$   & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.25,0.68]$ &   $4.9994$ &  $-20.1727$ & $  49.0418$ & $ -27.5918$ &   $ 0.9465$ &   $-0.4491$ &   $-0.0166$ &   $197$ & $1.5$\\
$V$   & $V-I_{\rm C}$   & $[-5.0,0.3]$ &  $[0.48,1.47]$ &   $3.4468$ &  $ -3.8760$ & $   4.5692$ & $  -0.7285$ &   $ 0.1832$ &   $-0.2991$ &   $-0.0231$ &   $184$ & $0.8$\\
$V$   & $V-J$     & $[-5.0,0.4]$ &  $[0.73,2.21]$ &   $1.8195$ &  $  1.5562$ & $  -1.3322$ & $   0.5627$ &   $ 0.1249$ &   $-0.3112$ &   $-0.0213$ &   $314$ & $0.8$\\
$V$   & $V-H$     & $[-5.0,0.4]$ &  $[0.67,3.01]$ &   $2.0139$ &  $  1.0845$ & $  -0.8071$ & $   0.2761$ &   $ 0.0567$ &   $-0.2147$ &   $-0.0124$ &   $369$ & $0.9$\\
$V$   & $V-K_{\rm S}$   & $[-5.0,0.4]$ &  $[0.93,3.15]$ &   $1.7662$ &  $  1.4154$ & $  -0.9302$ & $   0.2726$ &   $ 0.0692$ &   $-0.2506$ &   $-0.0160$ &   $316$ & $0.9$\\
$R_{\rm C}$ & $B-V$     & $[-5.0,0.3]$ &  $[0.35,1.29]$ &   $2.5759$ &  $ -1.8536$ & $   1.3042$ & $   0.1015$ &   $-0.0130$ &   $-0.1229$ &   $-0.0142$ &   $179$ & $0.8$\\
$R_{\rm C}$ & $V-R_{\rm C}$   & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.7031$ &  $ -4.2859$ & $   6.9274$ & $  -2.1959$ &   $ 0.1482$ &   $-0.1968$ &   $-0.0186$ &   $180$ & $0.7$\\
$R_{\rm C}$ & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.23,0.68]$ &   $3.2131$ &  $ -8.5410$ & $  17.3691$ & $  -9.1350$ &   $ 0.4602$ &   $-0.3054$ &   $-0.0171$ &   $203$ & $1.0$\\
$R_{\rm C}$ & $V-I_{\rm C}$ & $[-5.0,0.3]$ &  $[0.48,1.47]$ &   $2.9759$ &  $ -3.2013$ & $   2.9454$ & $  -0.6516$ &   $ 0.1331$ &   $-0.2408$ &   $-0.0187$ &   $185$ & $0.7$\\
$R_{\rm C}$ & $V-J$ & $[-5.0,0.3]$ &  $[0.86,2.36]$ &   $2.5806$ &  $ -1.0234$ & $   0.4055$ & $   0.0107$ &   $ 0.0874$ &   $-0.2508$ &   $-0.0181$ &   $184$ & $0.7$\\
$R_{\rm C}$ & $V-H$ & $[-5.0,0.3]$ &  $[0.93,2.99]$ &   $2.5007$ &  $ -0.6801$ & $   0.1842$ & $   0.0176$ &   $ 0.0746$ &   $-0.2604$ &   $-0.0185$ &   $196$ & $0.7$\\
$R_{\rm C}$ & $V-K_{\rm S}$ & $[-5.0,0.3]$ &  $[1.00,3.13]$ &   $2.5606$ &  $ -0.7448$ & $   0.2212$ & $   0.0049$ &   $ 0.0665$ &   $-0.2509$ &   $-0.0184$ &   $193$ & $0.7$\\
$I_{\rm C}$ & $B-V$ & $[-5.0,0.3]$ &  $[0.35,1.29]$ &   $2.6765$ &  $ -3.8643$ & $   3.7834$ & $  -1.2273$ &   $ 0.0145$ &   $-0.0358$ &   $-0.0015$ &   $200$ & $1.0$\\
$I_{\rm C}$ & $V-R_{\rm C}$ & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.6963$ &  $ -6.8081$ & $  11.3579$ & $  -6.1859$ &   $ 0.1798$ &   $-0.1418$ &   $-0.0112$ &   $191$ & $1.1$\\
$I_{\rm C}$ & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.27,0.68]$ &   $3.1500$ &  $-10.0132$ & $  18.2682$ & $ -10.8668$ &   $ 0.3653$ &   $-0.2329$ &   $-0.0123$ &   $177$ & $0.9$\\
$I_{\rm C}$ & $V-I_{\rm C}$ & $[-5.0,0.3]$ &  $[0.48,1.47]$ &   $3.0203$ &  $ -4.5225$ & $   4.0375$ & $  -1.1781$ &   $ 0.1371$ &   $-0.1866$ &   $-0.0122$ &   $197$ & $0.8$\\
$I_{\rm C}$ & $V-J$ & $[-5.0,0.3]$ &  $[0.86,2.36]$ &   $2.7912$ &  $ -2.2548$ & $   1.1687$ & $  -0.1986$ &   $ 0.0817$ &   $-0.1908$ &   $-0.0118$ &   $186$ & $1.1$\\
$I_{\rm C}$ & $V-H$ & $[-5.0,0.3]$ &  $[0.93,2.99]$ &   $2.7888$ &  $ -1.8271$ & $   0.7688$ & $  -0.1061$ &   $ 0.0734$ &   $-0.2132$ &   $-0.0138$ &   $187$ & $1.0$\\
$I_{\rm C}$ & $V-K_{\rm S}$ & $[-5.0,0.3]$ &  $[1.00,3.13]$ &   $2.7797$ &  $ -1.7014$ & $   0.6710$ & $  -0.0868$ &   $ 0.0603$ &   $-0.1891$ &   $-0.0123$ &   $193$ & $0.9$\\
$J$ & $B-V$ & $[-5.0,0.4]$ &  $[0.30,1.29]$ &   $2.2253$ &  $ -3.5932$ & $   2.9303$ & $  -0.8741$ &   $ 0.0199$ &   $ 0.0132$ &   $ 0.0057$ &   $346$ & $3.4$\\
$J$ & $V-R_{\rm C}$ & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.5765$ &  $ -8.1969$ & $  12.1713$ & $  -6.3037$ &   $ 0.1393$ &   $-0.0769$ &   $-0.0048$ &   $186$ & $2.9$\\
$J$ & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.27,0.68]$ &   $2.9723$ &  $-10.6481$ & $  16.3430$ & $  -8.5334$ &   $ 0.2971$ &   $-0.1854$ &   $-0.0095$ &   $195$ & $3.0$\\
$J$ & $V-I_{\rm C}$ & $[-5.0,0.3]$ &  $[0.52,1.47]$ &   $2.8966$ &  $ -5.1154$ & $   4.0119$ & $  -1.0879$ &   $ 0.1059$ &   $-0.1232$ &   $-0.0066$ &   $192$ & $2.6$\\
$J$ & $V-J$ & $[-5.0,0.4]$ &  $[0.82,2.44]$ &   $2.7915$ &  $ -2.8096$ & $   1.2799$ & $  -0.2049$ &   $ 0.0479$ &   $-0.1059$ &   $-0.0054$ &   $308$ & $0.8$\\
$J$ & $V-H$ & $[-5.0,0.4]$ &  $[0.88,2.99]$ &   $2.5885$ &  $ -2.0262$ & $   0.7430$ & $  -0.0963$ &   $ 0.0587$ &   $-0.1577$ &   $-0.0092$ &   $303$ & $1.9$\\
$J$ & $V-K_{\rm S}$ & $[-5.0,0.4]$ &  $[0.93,3.13]$ &   $2.5578$ &  $ -1.8710$ & $   0.6433$ & $  -0.0785$ &   $ 0.0457$ &   $-0.1326$ &   $-0.0078$ &   $314$ & $1.7$\\
$H$ & $B-V$ & $[-5.0,0.4]$ &  $[0.18,1.29]$ &   $2.1337$ &  $ -3.6473$ & $   2.6261$ & $  -0.6782$ &   $-0.0780$ &   $ 0.1274$ &   $ 0.0179$ &   $331$ & $4.6$\\
$H$ & $V-R_{\rm C}$ & $[-5.0,0.3]$ &  $[0.24,0.79]$ &   $2.5341$ &  $ -8.8850$ & $  12.8801$ & $  -6.5281$ &   $ 0.0339$ &   $-0.0012$ &   $ 0.0022$ &   $184$ & $3.6$\\
$H$ & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.23,0.68]$ &   $2.9097$ &  $-11.1909$ & $  16.5901$ & $  -8.3344$ &   $ 0.1844$ &   $-0.1169$ &   $-0.0047$ &   $192$ & $3.6$\\
$H$ & $V-I_{\rm C}$ & $[-5.0,0.3]$ &  $[0.48,1.47]$ &   $2.8833$ &  $ -5.5447$ & $   4.2495$ & $  -1.1267$ &   $ 0.0504$ &   $-0.0512$ &   $-0.0009$ &   $195$ & $3.1$\\
$H$ & $V-J$ & $[-5.0,0.4]$ &  $[0.50,2.44]$ &   $2.5764$ &  $ -2.6119$ & $   1.0580$ & $  -0.1490$ &   $ 0.0033$ &   $-0.0098$ &   $ 0.0031$ &   $353$ & $2.8$\\
$H$ & $V-H$ & $[-5.0,0.4]$ &  $[0.88,3.01]$ &   $2.4574$ &  $ -2.0093$ & $   0.6768$ & $  -0.0808$ &   $ 0.0246$ &   $-0.0665$ &   $-0.0016$ &   $344$ & $1.0$\\
$H$ & $V-K_{\rm S}$ & $[-5.0,0.4]$ &  $[0.57,3.15]$ &   $2.3732$ &  $ -1.7778$ & $   0.5485$ & $  -0.0599$ &   $ 0.0140$ &   $-0.0407$ &   $ 0.0005$ &   $363$ & $2.2$\\
$K_{\rm S}$ & $B-V$ & $[-5.0,0.4]$ &  $[0.30,1.29]$ &   $2.1537$ &  $ -3.9640$ & $   3.0680$ & $  -0.8653$ &   $-0.0586$ &   $ 0.1098$ &   $ 0.0163$ &   $353$ & $4.9$\\
$K_{\rm S}$ & $V-R_{\rm C}$ & $[-5.0,0.3]$ &  $[0.24,0.76]$ &   $2.5709$ &  $ -9.5441$ & $  14.4103$ & $  -7.6430$ &   $ 0.0585$ &   $-0.0186$ &   $ 0.0006$ &   $190$ & $3.8$\\
$K_{\rm S}$ & $(R-I)_{\rm C}$ & $[-5.0,0.3]$ &  $[0.25,0.68]$ &   $2.8803$ &  $-11.4591$ & $  17.4060$ & $  -9.0419$ &   $ 0.2418$ &   $-0.1469$ &   $-0.0066$ &   $199$ & $3.6$\\
$K_{\rm S}$ & $V-I_{\rm C}$ & $[-5.0,0.3]$ &  $[0.48,1.47]$ &   $2.7928$ &  $ -5.4377$ & $   4.1682$ & $  -1.1105$ &   $ 0.0661$ &   $-0.0690$ &   $-0.0019$ &   $201$ & $3.2$\\
$K_{\rm S}$ & $V-J$ & $[-5.0,0.4]$ &  $[0.50,2.36]$ &   $2.6548$ &  $ -2.8832$ & $   1.2411$ & $  -0.1878$ &   $ 0.0146$ &   $-0.0315$ &   $ 0.0013$ &   $328$ & $2.9$\\
$K_{\rm S}$ & $V-H$ & $[-5.0,0.4]$ &  $[0.88,2.99]$ &   $2.4939$ &  $ -2.1600$ & $   0.7593$ & $  -0.0946$ &   $ 0.0342$ &   $-0.0879$ &   $-0.0029$ &   $317$ & $2.5$\\
$K_{\rm S}$ & $V-K_{\rm S}$ & $[-5.0,0.4]$ &  $[0.93,3.03]$ &   $2.5097$ &  $ -2.0732$ & $   0.6972$ & $  -0.0836$ &   $ 0.0229$ &   $-0.0641$ &   $-0.0017$ &   $328$ & $1.1$\\
\hline 
\end{tabular}
\tablefoot{$N$ is the number of stars employed for the fit after the $3$ sigma
clipping and $\sigma(\%)$ is the standard deviation of the final calibrations in percent. The coefficients of the calibrations $b_i$ are given in units of $10^{-5}~{\rm erg~cm^{-2}~s^{-1}}$.}
%\vspace*{0.1mm}
\end{table}