\begin{table}%t1
%\centering
\par
\caption{\label{table:lowd}Overview and results of all the simulations.}
\begin{tabular}{l l l l l l l l l }        
\hline\hline\noalign{\smallskip}                 
Model& $\rho_{\rm g}$ & $\alpha$ & $r_{{\rm m}}$	&$\max (\bar{m})$	&$\max (\bar{\Psi})$	&$\Psi _{{\rm min}}$	&$t_{{\rm noc}}$ & $\max (\bar{St})$\\    
	& [g~cm$^{-3}$]& & &[g]	&	&	&[yr]	&\\
(1)	&(2)&(3)&(4)&(5)&(6)&(7)&(8)&(9)\\
\hline  \noalign{\smallskip}                        
Lt1d-3m100	&$2.4 \times 10^{-11}$	&$10^{-3}$	&100	&$8\times 10^{-8}$		&7.27	&1.77	&$2\times 10^{4}$	&$2.5\times 10^{-4}$	\\
Lt1d-4m100	&$2.4 \times 10^{-11}$	&$10^{-4}$	&100	&$9.7 \times 10^{-8}$	&7.12	&2.23	&$8\times 10^{4}$	&$2.2 \times 10^{-4}$	\\
Lt1d-5m100	&$2.4 \times 10^{-11}$	&$10^{-5}$	&100	&$2.66 \times 10^{-7}$	&7.72	&3.78	&$3 \times 10^{5}$	&$2.1 \times 10^{-4}$\\
%\hline  
Mt1d-3m100	&$1.4\times 10^{-9}$	&$10^{-3}$	&100	&8.13				&24.41	&3.88	&$10^{4}$		&$5.1\times 10^{-4}$\\		
Mt1d-4m100	&$1.4\times 10^{-9}$	&$10^{-4}$	&100	&4.18				&21.9	&1.85	&$2\times 10^5$	&$2.8 \times 10^{-4}$\\		
Mt1d-5m100	&$1.4\times 10^{-9}$	&$10^{-5}$	&100	&$7.7\times 10^{-2}$	&30.0	&4.13	&$7\times 10^{5}$	&$2.1\times 10^{-4}$\\
%\hline
Ht1d-3m100	&$2.7\times 10^{-8}$	&$10^{-3}$	&100	&3.77				&34.1	&5.61	&$10^5$			&$1.4 \times 10^{4}$\\		
Ht1d-4m100	&$2.7\times 10^{-8}$	&$10^{-4}$	&100	&0.23				&38.0	&5.41	&$3\times 10^6$	&$3.6\times 10^{-5}$\\		
Ht1d-5m100	&$2.7\times 10^{-8}$	&$10^{-5}$	&100	&0.28				&43.9	&4.94	&$4\times 10^6$	&$7.7\times 10^{-5}$\\
%\hline
Lt1d-4m10	&$2.4 \times 10^{-11}$	&$10^{-4}$	&10		&$9.2\times 10^{-4}$	&5.88	&2.28	&$10^5$			&$3.8 \times 10^{-3}$	\\
Lt1d-4m100	&$2.4 \times 10^{-11}$	&$10^{-4}$	&100	&$9.7 \times 10^{-8}$	&7.12	&2.23	&$8\times 10^{4}$	&$2.2 \times 10^{-4}$	\\
Lt1d-4m1000	&$2.4 \times 10^{-11}$	&$10^{-4}$	&1000	&$9.7 \times 10^{-8}$	&7.09	&2.29	&$8\times 10^{4}$	&$2.2 \times 10^{-4}$	\\
%\hline
Mt1d-4m10	&$1.4\times 10^{-9}$	&$10^{-4}$	&10		&$2.5\times 10^{-2}$	&19.4	&2.1		&$2\times 10^{5}$	&$2.2 \times 10^{-4}$\\
Mt1d-4m100	&$1.4\times 10^{-9}$	&$10^{-4}$	&100	&4.18				&21.9	&1.85	&$2\times 10^5$	&$2.8 \times 10^{-4}$\\		
Mt1d-4m1000	&$1.4\times 10^{-9}$	&$10^{-4}$	&1000	&$9.5 \times 10^{-3}$	&23.1	&2.9		&$2\times 10^{5}$	&$1.3\times 10^{-4}$\\
%\hline  
Ht1d-4m10	&$2.7\times 10^{-8}$	&$10^{-4}$	&10		&0.15				&34.6	&2.46	&$2\times 10^6$	&$4.5\times 10^{-5}$\\		
Ht1d-4m100	&$2.7\times 10^{-8}$	&$10^{-4}$	&100	&0.23				&38.0	&5.41	&$3\times 10^6$	&$3.6\times 10^{-5}$\\		
Ht1d-4m1000	&$2.7\times 10^{-8}$	&$10^{-4}$	&1000	&$8.8 \times 10^{-2}$	&40.0	&7.1		&$10^5$			&$3.5\times 10^{-5}$\\
\hline
\label{tab:res}
\end{tabular}
\tablefoot{In this table, Col.~1 describes the model names. ``L'' stands for the low density model, ``M'' is the MMSN model, ``H'' is the high density model, the letter ``t'' and the following number indicates the value of the turbulence parameter, the letter ``m'' and the number shows the used critical mass ratio values. Columns~2--4 shows the gas density, turbulence parameter, and the critical mass ratio respectively. Columns~5--9 list the parameters defined to characterize the distribution functions. These are the average maximum mass in Col.~5, the average maximum enlargement parameter in Col.~6, the minimum enlargement parameter in Col.~7, the end of the compaction phase in Col.~8, and the average maximum Stokes number in Col.~9.}
\end{table}