\begin{table}%tb12
%
\par
\caption{\label{tab:iras16347data}Photometric data for IRAS~16347+7037.}
\small%\centering
\par
{{\begin{tabular}{llll}
\hline\hline\noalign{\smallskip}
$\nu$ (Hz) & $F_{\nu}$ (Jy) & Error (Jy) & Ref. \\
\hline\noalign{\smallskip}
$1.45\times10^{9}$ & $9.40\times10^{-4}$ & $3.00\times10^{-4}$ & {VLA (NED)} \\ 
$1.49\times10^{9}$ & $1.65\times10^{-3}$ & $3.10\times10^{-4}$ & {VLA (NED)} \\ 
$4.90\times10^{9}$ & $1.08\times10^{-3}$ & $1.10\times10^{-4}$ & {VLA (NED)} \\ 
$8.48\times10^{9}$ & $9.70\times10^{-4}$ & $1.50\times10^{-4}$ & {VLA (NED)} \\ 
$1.49\times10^{10}$ & $1.17\times10^{-3}$ & $3.20\times10^{-4}$ & {VLA (NED)} \\ 
$2.25\times10^{10}$ & $9.60\times10^{-4}$ & $1.70\times10^{-4}$ & {VLA (NED)} \\ 
$4.00\times10^{10}$ & $2.78\times10^{-1}$ & ... & {FCRAO (NED)} \\ 
$9.00\times10^{10}$ & $4.50\times10^{-2}$ & ... & {NRAO-12m (NED)} \\ 
$2.30\times10^{11}$ & $1.50\times10^{-3}$ & ... & {IRAM (NED)} \\ 
$1.48\times10^{12}$ & $1.58\times10^{-1}$ & $3.16\times10^{-2}$ & {ISO (NED)} \\ 
$1.72\times10^{12}$ & $2.06\times10^{-1}$ & $4.12\times10^{-2}$ & {ISO (NED)} \\ 
$1.93\times10^{12}$ & $2.30\times10^{-1}$ & $4.60\times10^{-2}$ & {ISO (NED)} \\ 
$2.93\times10^{12}$ & $3.49\times10^{-1}$ & $6.98\times10^{-2}$ & {ISO (NED)} \\ 
$5.00\times10^{12}$ & $2.46\times10^{-1}$ & $3.20\times10^{-2}$ & {IRAS (NED)} \\ 
$1.20\times10^{13}$ & $1.22\times10^{-1}$ & $4.15\times10^{-3}$ & {IRAS (NED)} \\ 
$2.50\times10^{13}$ & $5.93\times10^{-2}$ & $1.01\times10^{-2}$ & {IRAS (NED)} \\ 
$2.52\times10^{13}$ & $4.80\times10^{-2}$ & $9.60\times10^{-3}$ & {ISO (NED)} \\ 
$2.97\times10^{13}$ & $4.90\times10^{-2}$ & $1.10\times10^{-2}$ & {Hale-5~m \citep{Neugebauer87}} \\ 
$8.10\times10^{13}$ & $1.07\times10^{-2}$ & $9.48\times10^{-4}$ & {Hale-5~m \citep{Neugebauer87}} \\ 
$1.39\times10^{14}$ & $6.99\times10^{-3}$ & $2.13\times10^{-4}$ & {2MASS} \\ 
$1.80\times10^{14}$ & $8.91\times10^{-3}$ & $2.75\times10^{-4}$ & {2MASS} \\ 
$2.43\times10^{14}$ & $6.96\times10^{-3}$ & $2.06\times10^{-4}$ & {2MASS} \\ 
$3.33\times10^{14}$ & $7.07\times10^{-3}$ & $1.95\times10^{-3}$ & {SSS} \\ 
$4.28\times10^{14}$ & $7.27\times10^{-3}$ & $2.01\times10^{-3}$ & {SSS} \\ 
$5.45\times10^{14}$ & $4.76\times10^{-3}$ & $4.00\times10^{-5}$ & {\XMM-OM} \\ 
$6.81\times10^{14}$ & $6.20\times10^{-3}$ & $2.28\times10^{-3}$ & {SSS} \\ 
$8.21\times10^{14}$ & $3.71\times10^{-3}$ & $1.60\times10^{-5}$ & {\XMM-OM} \\ 
$1.05\times10^{15}$ & $3.77\times10^{-3}$ & $4.97\times10^{-6}$ & {IUE} \\ 
$1.46\times10^{15}$ & $1.22\times10^{-3}$ & $4.71\times10^{-6}$ & {IUE} \\ 
$1.48\times10^{15}$ & $1.59\times10^{-3}$ & $6.00\times10^{-5}$ & {\XMM-OM} \\ 
$2.11\times10^{15}$ & $4.60\times10^{-4}$ & $8.92\times10^{-6}$ & {IUE} \\ 
 \hline 
\end{tabular} }}
\vspace*{7mm}
%\end{table}