\begin{table}%t2
\caption {\label{EjMass}Initial mass $M_{\rm ini}$, total released mass $M_{\rm rel}$, mass and fraction of ejected H ($M_{\rm H}$), He ($M_{\rm He}$), C ($M_{\rm C}$), N ($M_{\rm N}$), O ($M_{\rm O}$) and of heavy elements ($M_{\rm heavy}$), with all masses in ${M}_\odot$.}
%\centerline
 {
\begin{tabular}{ c c c c c c c c}
\hline\hline
$M_{\rm ini} $ &  $m_{\rm rel}$ & $m_{\rm H}$ & $m_{\rm He}$ & $m_{\rm C}$ & $m_{\rm N}$ & $m_{\rm O}$ & $m_{\rm heavy}$\\
\hline
\multicolumn{8}{c}{\vec{Z} {\bf = 0.004}}\\
$12$ & $10.4$ & $5.52~(53\%)$ & $4.30~(41\%)$ & $0.15~(1.4\%)$ & $1.7\times 10^{-2}~(0.16\%)$  & $8.9\times 10^{-2}~(0.86\%)$ & $0.58~(5.6\%)$\\
$15$ & $12.4$ & $6.11~(49\%)$ & $4.94~(40\%)$ & $0.25~(2.0\%)$ & $1.5\times 10^{-2}~(0.12\%)$ & $0.42~(3.4\%)$ & $1.35~(11\%)$\\
$20$ & $16.0$ & $6.57~(41\%)$ & $6.35~(40\%)$ & $0.49~(3.1\%)$ & $1.8\times 10^{-2}~(0.11\%)$  & $1.41~(8.8\%)$& $3.08~(19\%)$\\
$25$ & $17.5$ & $5.48~(31\%)$ & $7.09~(41\%)$ & $0.88~(5.0\%)$ & $2.1\times 10^{-2}~(0.12\%)$ & $2.64~(15\%)$ & 4.93~(28\%)\\
$30$ & $16.0$ & $1.58~(9.9\%)$ & $5.75~(36\%)$ & $1.45~(9.0\%)$ & $2.1\times 10^{-2}~(0.13\%)$  & $5.07~(32\%)$ & $8.67~(54\%)$\\
$40$ & $18.8$ & $0.45~(2.4\%)$ & $4.35~(23\%)$ & $2.11~(11\%)$ & $1.4\times 10^{-2}~(0.07\%)$ & $9.93~(53\%)$ & $14.0~(75\%)$\\
$60$ & $24.1$ & $0.00~(0.0\%)$ & $0.41~(1.7\%)$ & $2.16~(9.0\%)$ & $1.4\times 10^{-6}~(0.0\%)$  & $14.44~(60\%)$& $23.69~(98\%)$\\
$120$ & $13.8$ & $0.00~(0.0\%)$ & $0.48~(3.5\%)$ & $1.73~(13\%)$ & $0.00~(0.0\%)$  & $6.92~(50\%)$& $13.32~(97\%)$\\
\\
\multicolumn{8}{c}{\vec{Z} {\bf = 0.008}}\\
$20^1$ & $13.4$ & $9.70~(73\%)$ & $3.55~(27\%)$ & $2.4\times 10^{-2}~(0.18\%)$ & $7.5\times 10^{-3}~(0.06\%)$ & $5.6\times 10^{-2}~(0.42\%)$ & $0.11~(0.8\%)$\\ 
$25^1$ & $11.3$ & $7.83~(69\%)$ & $3.40~(30\%)$ & $1.6\times 10^{-2}~(0.14\%)$ & $1.5\times 10^{-2}~(0.14\%)$& $4.3\times 10^{-2}~(0.38\%)$ & $0.91~(0.8\%)$\\
$30$ & $9.2$ & $0.00~(0.0\%)$ & $0.54~(5.9\%)$ & $1.06~(12\%)$ & $1.8\times 10^{-3}~(0.02\%)$ & $3.30~(36\%)$ & $8.66~(94\%)$\\
$40$ & $13.9$ & $0.00~(0.0\%)$ & $0.31~(2.2\%)$ & $1.75~(13\%)$ & $3.0\times 10^{-4}~(0.0\%)$  & $6.98~(50\%)$& $13.59~(98\%)$\\
$60$ & $13.1$ & $0.00~(0.0\%)$ & $0.49~(3.7\%)$ & $1.68~(13\%)$ & $0.00~(0.0\%)$ & $6.48~(49\%)$ & $12.61~(96\%)$\\
$120$ & $10.4$ & $0.00~(0.0\%)$ & $0.44~(4.2\%)$ & $1.36~(13\%)$ & $0.00~(0.0\%)$ & $4.55~(44\%)$ & $9.96~(96\%)$\\
\\
\multicolumn{8}{c}{\vec{Z} {\bf = 0.020}}\\
$12$ & $9.1$ & $4.13~(45\%)$ & $4.20~(46\%)$ & $0.18~(2.0\%)$ & $5.4\times 10^{-2}~(0.59\%)$ & $0.18~(1.9\%)$ & $0.77~(8.5\%)$\\
$15$ & $8.5$ & $2.53~(30\%)$ & $3.83~(45\%)$ & $0.32~(3.7\%)$ & $5.0\times 10^{-2}~(0.59\%)$ & $0.84~(9.9\%)$ & $2.14~(25\%)$\\
$20$ & $9.8$ & $1.40~(14\%)$ & $3.51~(36\%)$ & $0.74~(7.6\%)$ & $4.7\times 10^{-2}~(0.48\%)$ & $2.22~(23\%)$ & $4.89~(50\%)$\\
$25$ & $8.8$ & $3.78\times 10^{-5}~(0.0\%)$ & $2.04~(23\%)$ & $1.13~(13\%)$ & $2.6\times 10^{-2}~(0.29\%)$ & $3.50~(40\%)$ & $6.76~(77\%)$\\
$40$ & $9.7$ & $0.00~(0.0\%)$ & $0.53~(5.5\%)$ & $1.21~(12\%)$ &  
$3.8\times 10^{-6}~(0.0\%)$ & $3.77~(39\%)$ & $9.17~(95\%)$\\
$60$ & $11.0$ & $0.00~(0.0\%)$ & $0.54~(4.9\%)$ & $1.43~(13\%)$ & $4.4\times 10^{-6}~(0.0\%)$  & $4.86~(44\%)$& $10.46~(95\%)$\\
$85$ & $9.3$ & $0.00~(0.0\%)$ & $0.53~(5.7\%)$ & $1.11~(12\%)$ & $3.7\times 10^{-6}~(0.0\%)$  & $3.43~(37\%)$& $8.77~(94\%)$\\
$120$ & $8.5$ & $0.00~(0.0\%)$ & $0.49~(5.8\%)$ & $0.96~(11\%)$ &  $3.4\times 10^{-6}~(0.0\%)$ & $2.94~(35\%)$& $8.01~(94\%)$\\
\\
\multicolumn{8}{c}{\vec{Z} {\bf = 0.040}}\\
$20$ & $7.8$ & $7.1\times 10^{-2}~(0.91\%)$ & $1.96~(25\%)$ & $0.77~(9.9\%)$ & $4.62\times 10^{-2}~(0.59\%)$ & $2.29~(29\%)$ & $5.77~(74\%)$\\
$25$ & $7.9$ & $0.00~(0.0\%)$ & $0.51~(6.5\%)$ & $0.65~(8.2\%)$ & $0.00~(0.0\%)$ & $1.88~(24\%)$ & $7.39~(94\%)$\\
$40$ & $8.6$ & $0.00~(0.0\%)$ & $0.41~(8.3\%)$ & $1.00~(12\%)$ & $0.00~(0.0\%)$ & $3.07~(36\%)$ & $7.89~(92\%)$\\
$85$ & $5.0$ & $0.00~(0.0\%)$ & $0.48~(9.6\%)$ & $0.33~(6.6\%)$ & $0.00~(0.0\%)$ & $0.89~(18\%)$ & $4.52~(90\%)$\\
$120$ & $4.9$ & $0.00~(0.0\%)$ & $0.44~(9.0\%)$ & $0.33~(6.8\%)$ & $0.00~(0.0\%)$ & $0.90~(18\%)$ & $4.46~(91\%)$\\
\hline
\multicolumn{8}{c}{\textbf{Homogenous model at} \vec{Z} {\bf = 0.002}}\\
$60^2$ & $23.8$ & $0.00~(0.0\%)$ & $0.64~(2.7\%)$ & $2.33~(9.8\%)$ & $3.66\times 10^{-7}~(0.0\%)$ & $15.56~(65\%)$ & $23.12~(97\%)$\\
\hline
\end{tabular}}
\par
\smallskip
{(1) See note (1) in Table~\ref{HeMass}.}\\
{(2) Model computed up to the end of silicon burning.}\\
\end{table}