\begin{table}%t6
\caption{\label{tab:MWC480}Observed fluxes for MWC480.}
%\centering
 \small \begin{tabular}{lcll}
\hline\hline\noalign{\smallskip}
Type & $\lambda$ & Flux & Reference \\
\hline \noalign{\smallskip}
O~{\sc i} & 63~$\mu$m & $\leqslant$$ 1.1\times 10^{-15}$~W/m$^2$/$\mu$m &  1  \\[2mm]
O~{\sc i} & 145~$\mu$m & $\leqslant$$ 1.8\times 10^{-16}$~W/m$^2$/$\mu$m &  {1} \\[2mm]
C~{\sc ii} & 158~$\mu$m & $5.9\pm 0.6\times 10^{-16}$~W/m$^2$ &  {1} \\
 & & $5.5\pm 0.4\times 10^{-16}$~W/m$^2$ &  {2} \\[2mm]
CO  &  345~GHz & 2.88~K~km~s$^{-1}$ &  {3} \\
    &   & $4.23\times 10^{-19}$~W/m$^2$ &  {*} \\[2mm]
cont. &  1.3~mm & $360\pm24$~mJy &  {4} \\
cont. &  2.7~mm & $39.9\pm 0.8$~mJy &  {4} \\
\hline
\end{tabular}
\tablebib{(1) \citet{Creech2002}; (2) \citet{Lorenzetti2002};  (3)~\citet{Thi2004};  (4)  \citet{Mannings1997a}. (*)~$\int T_{\rm mb}~{\rm d}v = 10^{-2} ~ \lambda_{\rm cm}/(2k) ~ (\Omega_a)^{-1}  \int F_\nu({\rm W/m^2/Hz})~{\rm d}\nu$, with $\Omega_a$ being the solid angle of the beam, i.e. $\pi (13.7''/2)^2$ for the JCMT.}
\end{table}