\begin{table}%t3
\caption{\label{summary_table}Summary of the burst properties of five \textit{Fermi}/LAT bursts.} 
\par
%\centering
\par
\begin{tabular}{lccccccccc} 
\hline\hline \noalign{\smallskip}
Burst  &  Redshift  & $E_{\gamma, \rm{iso}}$$^1$  
 & $\alpha$ &  $\beta_{\rm opt}$  &  Template & $A_{V}^{\rm{host}}$ &  $\theta_{\rm jet}^{\rm ISM}$  &$E_{\rm{\gamma}}$$^a$ %\footnotemark[a] 
   & SFR$^b$ %\footnotemark[b] 
    \\
 	&	& erg	&		&	&		& & 	 {\it $^\circ$}  &  {(erg)}    & {($M_\odot$ yr$^{-1}$)}  \\
\hline \noalign{\smallskip}
GRB~090323$^c$ %\footnotemark[c] 
& 3.57$^{1}$ & $5.1\times 10^{54}$ & $1.90\pm0.01$ & $0.65\pm0.13$ & SMC & $0.14^{\rm +0.04}_{-0.03}$ & ${\la}2.1^\circ$ & ${\la}3.3 \times 10^{51}$ & $\cdots$ \\
GRB~090328 & 0.7354 & $1.0\times 10^{53}$ & $2.27\pm{0.04}$ & $1.19^{\rm +0.24}_{-0.21}$ & SMC & $0.22^{\rm +0.06}_{-0.18}$ & ${\la}5.5^\circ$ & ${\la}4.6 \times 10^{50}$	&  4.8  \\
GRB~090902B & 1.822$^{2}$ & $3.5\times 10^{54}$ & $0.94 \pm 0.02$ & $0.79^{\rm +0.05}_{-0.19}$ & SMC/LMC & ${\la}0.34$  & ${\ga}6.4^\circ$ &  ${\ga}2.2 \times 10^{52}$ 	& $\cdots$    \\
GRB~080916C$^{3}$,$^c$%\footnotemark[c] \footnotemark[c]
  & 4.35$^{3}$ & $8.8\times 10^{54}$ & $ 1.40 \pm 0.05$ & $0.38^{\rm +0.20}_{-0.19}$ & $\cdots$ &  $\cdots$  & ${\ga}6^\circ$ &  ${\ga}4.8 \times 10^{52}$ 	& $\cdots$    \\
GRB~090510 & 0.903 & $1.1\times 10^{53}$ & $\cdots$ & $\cdots$ & $\cdots$ & $\leq$1.1 & $\cdots$ & $\cdots$ & 0.30 \\
\hline
\end{tabular}
\tablebib {(1) \citet{2009GCN..9028....1C}; (2) \citet{Z_090902B}; (3) \citet{2009AetA...498...89G}.
}
\tablefoot {\tablefoottext{a}{$E_{\gamma, \rm{iso}}$ values are  quoted in the energy range 1~keV$-$10~GeV, with the exception of  GRB~080916C (10~keV$-$10~GeV: \citealt{2009arXiv0908.1832F}) and GRB~090510  (10~keV$-$30~GeV: \citealt{090902B_PAPER}).}
\tablefoottext{b}{The true SFR may be larger than measured because of slit losses.}
\tablefoottext{c}{The opening angle and $E_{\rm{\gamma}}$  are lower in a wind medium for GRB~090323 and~080916C.}}
\vspace*{2.5mm}
\end{table}