\begin{table}%t2
\caption{\label{tab:specs300}Spectral fit of the measured VHE spectra extracted in different epochs (see Table~1). }
%\centering
\par
\begin{tabular}{lccccccc}
\hline
\hline
%\\
PL fits  &   $\Phi_0$ & $\Gamma$   &       &          & $F_{0.3-3~\rm TeV}$ &     $\chi^2_r$ (d.o.f.) & $P_{{\chi}^2}$ \\
         &  cm$^{-2}$~s$^{-1}$~TeV$^{-1}$&  &&          & erg cm$^{-2}$ s$^{-1}$ &         &      \\
\hline
\\
\par
\texttt{T400-Peak}   &2.20~$\pm$~0.06\e{-10} &3.46~$\pm$~0.04 &--&--& 1.35\e{-09} & 3.66 (11) & 3\e{-5}\\
\texttt{T300-High}   &1.36~$\pm$~0.03\e{-10} &3.36~$\pm$~0.03 &--&--& 7.88\e{-10} & 4.3 (12)  & 7\e{-7}\\
\texttt{T300-Low}    &4.89~$\pm$~0.15\e{-11} &3.51~$\pm$~0.03 &--&--& 3.09\e{-10} & 1.36 (12) & 0.18\\
\texttt{T200}        &7.46~$\pm$~0.12\e{-11} &3.25~$\pm$~0.01 &--&--& 4.06\e{-10} & 16 (16)   & 0\\
\texttt{T300-RXTE}   &4.78~$\pm$~0.30\e{-11} &3.53~$\pm$~0.07 &--&--& 3.07\e{-10} & 1.4 (11)  & 0.17\\
\par
\hline
%\hline
%\\
PL exp. cut. &$\Phi_0$       &   $\Gamma$ & $E_{\rm cut}$(TeV)  &       &  $F_{0.3{-}3~\rm TeV}$ &     $\chi^2_r$ (d.o.f.) & $P_{{\chi}^2}$ \\
%           &              &   TeV      &    & cm$^{-2}$s$^{-1}$TeV$^{-1}$ & ergs cm$^{-2}$ s$^{-1}$ &          &       \\ 
 \\ 
\par
\texttt{T400-Peak} &5.96~$\pm$~1.19\e{-10} &2.60~$\pm$~0.17 &1.19~$\pm$~0.25 &--& 1.28\e{-09} &0.38 (10) & 0.96\\
\texttt{T300-High} &2.72~$\pm$~0.36\e{-10} &2.86~$\pm$~0.09 &1.66~$\pm$~0.33 &--& 7.95\e{-10} &1.41 (11)  & 0.16\\
\texttt{T300-Low}  &7.08~$\pm$~1.25\e{-11} &3.26~$\pm$~0.12 &2.92~$\pm$~1.42 &--& 3.08\e{-10} &0.98 (11) & 0.47\\
\texttt{T200}      &2.12~$\pm$~0.23\e{-10} &2.65~$\pm$~0.06 &1.01~$\pm$~0.11 &--& 4.25\e{-10} &4.41 (15)  & 2\e{-8}\\
%TRXTE     &5.86$\pm$0.39\e{-11} &3.4$\pm$0.075 &5.0$\pm$4.79  &-& 3.06\e{-10} &1.56 (10) & 0.112\\			       
\hline
%\hline
%\\
Log-parabolic &$\Phi_0$      &   $\Gamma$  &  $b$   &    &   $F_{0.3-3~\rm TeV}$ &     $\chi^2_r$ (d.o.f.) & $P_{{\chi}^2}$ \\
\par
%              &             &        &   & cm$^{-2}$s$^{-1}$TeV$^{-1}$ & ergs cm$^{-2}$s$^{-1}$ &          &       \\ 
 \\ 
\par
\texttt{T400-Peak}  &2.55~$\pm$~0.09\e{-10} &3.54~$\pm$~0.06 &1.05~$\pm$~0.20  &--& 1.25\e{-09} & 0.37 (10) & 0.96\\
\texttt{T300-High}  &1.46~$\pm$~0.04\e{-10} &3.53~$\pm$~0.05 &0.62~$\pm$~0.11  &--& 7.94\e{-10} & 1.35 (11) & 0.19\\
\texttt{T300-Low}   &4.98~$\pm$~0.16\e{-11} &3.66~$\pm$~0.07 &0.41~$\pm$~0.16  &--& 3.08\e{-10} & 0.76 (11) & 0.68\\
\texttt{T200}       &7.51~$\pm$~0.16\e{-11} &3.69~$\pm$~0.05 &0.78~$\pm$~0.07  &--& 4.29\e{-10} & 2.39 (15) & 0.002\\
%TRXTE      &4.77$\pm$0.31\e{-11} &3.62$\pm$0.18 &0.19$\pm$0.35  &-&3.07\e{-10} & 1.51 (10) & 0.129\\
\par
\hline
%\hline
%\\
Broken PL   & $\Phi_0$        &   $\Gamma_1$  &$\Gamma_2$   & $E_{\rm break}$(TeV)  &   $F_{0.3-3~\rm TeV}$ & $\chi^2_r$ (d.o.f.)  &$P_{{\chi}^2}$ \\
%           &                &    TeV         &           & cm$^{-2}$s$^{-1}$TeV$^{-1}$ & ergs cm$^{-2}$ s$^{-1}$ &          &    \\ 
 \\ 
\texttt{T200}    &1.46~$\pm$~0.10\e{-10}  &2.73~$\pm$~0.05  & 3.60~$\pm$~0.04 & 0.42~$\pm$~0.02 & 4.31\e{-10} & 1.44 (14) & 0.12\\
%\par
% \\
\hline
\end{tabular}
\end{table}