\begin{table}%T4
\caption{\label{param}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. (\cite{Ghisellini2002}). Below the dividing line we 
list the output parameters for the four fitted sources. See the text for more details.} 
\small%\centering
\par
\begin{tabular}{llllll}
\hline\hline
Parameter            & AO~$0235+164$ & PKS~$1334-127$ & PKS~$1406-076$  & PKS~$1830-211$ & Units \\
\hline\noalign{\smallskip}
$R$                  & $4.5$         & $3.5$          & $2.0$           & $2.0$           & $10^{16}$~cm \\
$\Delta R$           & $2.8$         & $3.5$          & $2.0$           & $30$            & $10^{15}$~cm \\
$L^\prime_{\rm inj}$ & $7.5$         & $3.0$          & $3.0$           & $7.0$           & $10^{43}$~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 \\
$\delta$             & $18.2$        & $9.6$          & $14.3$          & $16.4$          &  \\
$L_{\rm BLR}$            & $3.0$         & $4.5$          & $0.8$           & $12$            & $10^{44}$~erg~s$^{-1}$  \\
$R_{\rm BLR}$            & $7.0$         & $3.5$          & $5.0$           & $3.5$           & $10^{17}$~cm \\\noalign{\smallskip}
\hline\noalign{\smallskip}
$\gamma_{\rm peak}$  & $2.0\times 10^{4}$ & $2.5\times 10^{2}$ & $1.6\times 10^{3}$       & $1.4\times 10^{2}$   & \\
$U_B$                & $0.067$       & $0.54$         & $0.04$          & $0.57$          & erg~cm$^{-3}$\\
$U^\prime_{\rm r}(\gamma_{\rm peak})$ & $0.042$ & $1.8$ & $0.25$        & $10.87$         & erg~cm$^{-3}$\\
$L_B$                & $3.28$        & $6.26$         & $0.15$          & $14$            & $10^{45}$~erg~s$^{-1}$\\
$L_{\rm e}$          & $1.05$        & $1.78$         & $8.8$           & $1.0$           & $10^{45}$~erg~s$^{-1}$\\
$L_{\rm p}$          & $7.16$        & $3.15$         & $25$            & $26.5$          & $10^{46}$~erg~s$^{-1}$\\
$L_{\rm rad}$        & $4.588$       & $3.59$         & $3.2$           & $20.8$          & $10^{45}$~erg~s$^{-1}$\\
\hline
\end{tabular}
\end{table}