\begin{table}%t2
\caption{Some results for the torus evolution models. The
dynamical simulations were performed over a time interval of $\Delta
t_{\rm cal}$. All quantities refer to the conditions found at the
end of the simulations. $M_{\rm d}$ is the mass of the gas of the
disk, $T_{\rm max}$ is the maximum gas temperature in energy units,
$L_{\nu_{\rm e}}$ denotes the electron neutrino luminosity near the end of
the simulation, $L_{\bar{\nu}_{\rm e}}$ the corresponding electron
antineutrino luminosity, and $L_{\nu_x}$ the luminosity of
heavy-lepton neutrinos (summed for $\nu_{\mu}$,
$\bar\nu_{\mu}$, $\nu_{\tau}$ or $\bar\nu_{\tau}$, which are all
treated equally). The sum of all neutrino luminosities is given by
$L_\nu$, and the mean energies of the different neutrino types by
$\langle\epsilon_{\nu_{\rm e}}\rangle$,
$\langle\epsilon_{\bar{\nu}_{\rm e}}\rangle$ and
$\langle\epsilon_{\nu_x}\rangle$. }
%\begin{flushleft}
%%\begin{center}

\par
\begin{tabular}{llcccccccrr}
\hline\hline 
Model & $\Delta t_{\rm cal}$ &
   $M_{\rm d}$ & $T_{\rm max}$ &
   $L_{\nu_{\rm e}}$ & $L_{\bar{\nu}_{\rm e}}$ & $L_{\nu_x}$ & $L_\nu$ &
   $\langle\epsilon_{\nu_{\rm e}}\rangle$ &
   $\langle\epsilon_{\bar{\nu}_{\rm e}}\rangle$ &
   $\langle\epsilon_{\nu_x}\rangle$ \\
 & ms &
   {\scriptsize$10^{-2}M_\odot$} & {\scriptsize MeV} &
   {\scriptsize$10^{50}\frac{\rm erg}{\rm s}$} &
   {\scriptsize$10^{50}\frac{\rm erg}{\rm s}$} &
   {\scriptsize$10^{50}\frac{\rm erg}{\rm s}$} &
   {\scriptsize$10^{50}\frac{\rm erg}{\rm s}$} &
   {\scriptsize MeV} & {\scriptsize MeV} & {\scriptsize MeV}
\\[0.3ex] \hline 
r00-32  & 70.0 & 1.06 & 2.6
    &  0.08 & 0.22  & 0.002 & 0.3 & 9.7 & 9.3 & 7.8     \\   %0.0   32
al1-32  & 70.0 & 1.14 & 3.3
    &  0.2  & 0.6   & 0.01  & 0.8 &12.5 &12.0 &10.0     \\   %0.001 32
al2-32  & 70.0 & 1.25 & 4.3
    &  1.0  & 2.9   & 0.1   & 4.0 &15.4 &15.2 &12.8     \\   %0.004 32
al3-32  & 70.0 & 1.43 & 5.0
    &  1.4  & 3.9   & 0.2   & 5.5 &17.5 &17.2 &14.7     \\   %0.01  32
al4-32  & 70.0 & 0.84 & 5.9
    &  4.0  & 9.0   & 2.0   &15.0 &17.5 &19.2 &16.9     \\   %0.1   32
ro1-32  & 70.0 & 1.54 & 3.8
    &  0.3  & 0.8  & 0.008 & 1.1 & 11.3 & 11.0 & 9.4    \\   % pro 0.3  32
ro2-32  & 70.0 & 2.10 & 4.5
    &  0.7  & 1.8  & 0.03 & 2.5 & 11.4 & 11.2 & 9.7    \\   % pro 0.6  32
ro3-32  & 70.0 & 2.02 & 6.4
    &  9.0  & 14.0  & 0.4 &23.0 & 18.2 & 19.1 & 18.3  \\   % pro 0.8  32
ro4-32  & 70.0 & 0.67 & 2.1
    & 0.009 & 0.02 & 0.0006 & 0.03 & 8.5 & 8.3 & 6.9  \\   % ret 0.3  32
ro5-32  & 70.0 & 0.56 & 1.8
    & $<$0.005 & $<$0.01 & $<$0.0002 & $<$0.015 & 5.8 & 6.1 & 5.4      \\   %  ret 0.6  32
ir1-32  & 70.0 & 0.46 & 1.4
    & $<$0.0005  & $<$0.0005  & $<$0.0001 & $<$0.001 & 5.1 & 5.6 & 4.7  \\   %  1/4  32
ir2-32  & 70.0 & 0.57 & 1.9
    & $<$0.0025  & $<$0.0025  & $<$0.0005 & $<$0.005 & 6.8 & 6.7 & 5.7  \\   %  1/2  32
ir3-32  & 70.0 & 2.35 & 3.1
    &  1.7 & 2.4  &0.035 &  4.1 & 11.9 & 11.4 & 9.6                     \\   %  2    32
ir4-32  & 70.0 & 4.31 & 7.1
    &  34.0 & 50.0 &2.0 & 86.0 & 17.3 & 17.3 & 17.0                        %  4    32
     \\[0.7ex]
r00-64 & 40.0 & 2.22 & 4.2
    &  0.6 &  1.2  & 0.01& 1.8 & 12.0 & 11.6 & 10.2 \\  %0.0  64
al3-64 & 40.0 & 2.44 & 5.6
    &  3.4 &  7.7 & 0.3   &11.4 & 16.4 & 17.8 & 15.4 \\  %0.01 64
al4-64 & 40.0 & 1.76 & 8.7
    & 18.0 & 55.0 & 7.0   &80.0 & 21.3 & 22.8 & 20.1 \\  %0.1  64
ri4-64 & 40.0 &12.22 & 7.0
    & 26.0 & 43.0 & 1.0 &70.0 & 14.5 & 16.5 & 17.9 \\  %  4  64
ro2-64 & 40.0 & 3.10 & 4.6
    &  1.6 & 1.8  & 0.02 & 3.4 & 12.9 & 11.7 & 11.7  \\  % pro 0.6  64
ro5-64 & 40.0 & 1.13 & 3.9
    &  0.3 & 0.7  & 0.01 & 1.0 & 12.2 & 11.8 &  9.8  \\  % ret 0.6  64
ir1-64 & 40.0 & 0.71 & 2.4
    & 0.07 & 0.03 & 0.001 & 0.1 &  9.4 &  8.4 & 7.0  \\  %  1/4  64
ir4-64 & 40.0 & 7.87 & 6.2
    &  7.2 & 15.0 & 0.2 &22.4 & 13.8 & 12.8 & 14.9 \\  %  4    64
ir5-64 & 40.0 & 8.77 & 10.4
    &150.0 &350.0 &110.0 &610.0 & 20.7 & 20.9 & 26.7 \\  %  4    64
ar1-64 & 40.0 & 2.34 & 6.6
    & 25.0 &70.0  &15.0  &110.0 & 21.5 & 22.7 & 20.3 \\  %  1 0.6 64
ar2-64 & 40.0 &10.44 & 9.5
    &120.0 &240.0 & 80.0 &440.0 & 19.4 & 19.7 & 25.2     %  4 0.6 64
     \\[0.7ex]
\hline
\end{tabular}
%%\end{center}

\par
%\end{flushleft}
\label{tab:models}
\end{table}