\begin{table}%t3
%\centering
\par
\caption {Masses and momenta of the outflows calculated from the $m_{\rm
H_2}(v)$ relation using the velocity ranges 2--40~\kms\ and 
7--40~\kms\ with 
a bin width of 1~\kms.  Also shown are $\langle v\rangle_{\rm lobe}$ and $v_{\rm max}$, 
the latter chosen as the velocity at which $I_{\rm CO}$ is $1/100$ that at 
$v_{\rm min}$ (see text).
\label{vmin-truncation-table}}
\begin{tabular}{ccccccccccc}\hline\hline
\noalign{\smallskip}
\multirow{2}{*}{$\eta$} & \multirow{2}{*}{$\alpha$} &
\multirow{2}{*}{$L_{\rm lobe}$ ($10^{-1}$ pc)} & \multicolumn{2}{c}{$\langle v\rangle_{\rm
	flow}$ (\kms)} & \multicolumn{2}{c}{$v_{\rm max}$ (\kms)} &
\multicolumn{2}{c}{$\displaystyle\frac{m_{\rm observed}}{m_{\rm H_2}}$} &
\multicolumn{2}{c}{$\displaystyle\frac{|P_{\rm blue}| + |P_{\rm red}|}{
P_{{\rm H_2}, z}}$} \\
 & & & (2--40) & (7--40)  & (2--40) & (7--40) & (2--40) & 
 (7--40) & (2--40) & (7--40) \\
\hline
\noalign{\smallskip}
\multirow{4}{*}{0.1} & $0^\circ$ & 0.91 & 2.68 & 8.82 &
6 & 17 & 0.33 & $3.0\times10^{-3}$ & 0.39 & $1.2\times10^{-2}$ \\
		& $30^\circ$ & 0.53 & 3.47 & 10.17 & 15 & 25 & 0.37 
		& $3.4\times10^{-2}$ & 0.56 & 0.15 \\
		& $60^\circ$ & 0.36 & 4.94 & 11.81 & 20 & 32 & 0.35 
		& $7.7\times10^{-2}$ & 0.76 & 0.41 \\
		& $90^\circ$ & 0.10 & 5.55 & 12.50 & 20 & 35 & 0.34 
		& $8.8\times10^{-2}$ & 0.85 & 0.50 \\ \hline
\multirow{4}{*}{1} & $0^\circ$ & 2.01 & 3.80 & 8.65 & 11
& 17 & 0.66 & $5.4\times10^{-2}$ & 1.72 & 0.32 \\
		& $30^\circ$ & 1.63 & 3.70 & 9.24 & 13 & 24 & 0.64 
		& $5.1\times10^{-2}$ & 1.61 & 0.32 \\
		& $60^\circ$ & 0.90 & 3.62 & 10.57 & 13 & 31 & 0.50 
		& $5.5\times10^{-2}$ & 1.26 & 0.41 \\
		& $90^\circ$ & 0.15 & 4.90 & 11.24 & 17 & 36 & 0.26 
		& $5.6\times10^{-2}$ & 0.89 & 0.45  \\ 
		\hline
\end{tabular}
\end{table}