\begin{table}%t1
%\centering
\par
\caption{\label{table1}\label{tab:modelos}Parameters of the collapse models and outcome of the
simulations.} 
\begin{tabular}{ccccccccc}
\hline\hline 
\noalign{\smallskip}
Initial configuration & Model & $\frac{R_{\rm c}}{R_0}$ & $\rho_{\rm av}$ &
$M_{\rm c}$ & $\Omega_{\rm c}$ & $c_0$ & $\rho_{\rm crit}$ & Outcome \\
 & & & $\rm gr ~ cm^{-3}$ & gr & $\times 10^{-13}$~rad/s  & cm/s  & $ \rm gr ~ cm^{-3}$ &
\\
\hline
\noalign{\smallskip} 
  IC0 & A0 & 0.5 & $2.23~ \times 10^{-18}$ &$6.28 \times 10^{32}$ &5.80
  & 10620.35 & $5.0~\times 10^{-14}$ & triple   \\
  IC0 & B0 & &  &  & &  & $5.0~\times 10^{-12}$ & filament \\
  IC1 & A1 & 1.5 & $6.95~ \times 10^{-19}$ &$5.14 \times 10^{33}$ & 3.90
  & 18751.51 & $5.0~\times 10^{-14}$ & quadruple\\
  IC1 & B1 & & & && & $5.0~\times 10^{-12}$ & single   \\
  IC2 & A2 & 2.5 & $2.43~ \times 10^{-19}$ &$8.34~ \times 10^{33}$ & 2.95
  & 19942.80 & $5.0~\times 10^{-14}$ & binary   \\
  IC2 & B2 & &  &  & &  & $5.0~\times 10^{-12}$ & single   \\
  IC3 & A3 & 3.7 & $9.22 ~ \times 10^{-20}$&$1.04 \times 10^{34}$& 2.22 &
  20344.14 & $5.0~\times 10^{-14}$ & binary   \\
  IC3 & B3 &  & &  && & $5.0~\times 10^{-12}$ & single   \\
\hline   
\end{tabular}
\end{table}