Table 4: Parameters for the models of AO 0235+164, PKS 1334-127, PKS 1406-076, and PKS 1830-211: above the dividing line are listed the input parameters used to model the SED according to the finite injection time synchrotron-inverse Compton model of Ghisellini et al. (2002). Below the dividing line we list the output parameters for the four fitted sources. See the text for more details.
Parameter AO 0235+164 PKS 1334-127 PKS 1406-076 PKS 1830-211 Units

R		 4.5 3.5 2.0 2.0 1016 cm
$\Delta R$ 2.8 3.5 2.0 30 1015 cm
$L^\prime_{\rm inj}$ 7.5 3.0 3.0 7.0 1043 erg s-1
$\gamma_{\rm break}$ $2.0\times 10^{4}$ $2.5\times 10^{2}$ $1.0\times 10^{2}$ $1.4\times 10^{2}$  
$\gamma_{\rm max}$ $6.0\times 10^{5}$ $4.0\times 10^{3}$ $5.0\times 10^{3}$ $1.6\times 10^{3}$  
s 2.55 2.7 2.2 2.8  
B 1.3 3.7 1.0 3.8 Gauss
$\Gamma $ 16 10 10 17  
$\theta$ 3 6 3.6 3.5 degree
$\delta $ 18.2 9.6 14.3 16.4  
$L_{\rm BLR}$ 3.0 4.5 0.8 12 1044 erg s-1
$R_{\rm BLR}$ 7.0 3.5 5.0 3.5 1017 cm

$\gamma_{\rm peak}$		 $2.0\times 10^{4}$ $2.5\times 10^{2}$ $1.6\times 10^{3}$ $1.4\times 10^{2}$  
UB 0.067 0.54 0.04 0.57 erg cm-3
$U^\prime_{\rm r}(\gamma_{\rm peak})$ 0.042 1.8 0.25 10.87 erg cm-3
LB 3.28 6.26 0.15 14 1045 erg s-1
$L_{\rm e}$ 1.05 1.78 8.8 1.0 1045 erg s-1
$L_{\rm p}$ 7.16 3.15 25 26.5 1046 erg s-1
$L_{\rm rad}$ 4.588 3.59 3.2 20.8 1045 erg s-1


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