\begin{table}%t5 \caption{\label{12745tb5}Supernovae type Ia mass fraction, $\xi = M_{\rm Fe,SNIa}/(M_{\rm Fe,SNIa}+M_{\rm Fe,SNcc})$, obtained for different theoretical SNe silicon-to-iron and nickel-to-iron ratios from the observed Si/Fe and Ni/Fe ratios. } \small%\centerline { \begin{tabular}{r| c c c c c c c} \hline\hline {\it mekal} model & & & & SNIa & & &\\ \hline SNcc & W7 & W70 & WDD1 & WDD2 & WDD3 & CDD1 & CDD2 \\ \hline No06,S &$0.528{-}0.571$&$0.515{-}0.734$&$ $&$ $&$ $&$ $&$ $ \\ No06,T &$0.575{-}0.579$&$0.562{-}0.760$&$ $&$ $&$ $&$ $&$ $ \\ CL04,S &$ $&$0.505{-}0.582$&$ $&$0.546{-}0.789$&$0.505{-}0.728$&$ $&$0.534{-}0.770$ \\ CL04,T &$ $&$0.559{-}0.728$&$ $&$0.600{-}0.727$&$0.559{-}0.758$&$ $&$0.588{-}0.727$ \\ W95,S &$ $&$ $&$0.616{-}0.677$&$0.518{-}0.775$&$0.476{-}0.712$&$0.635{-}0.652$&$0.505{-}0.756$ \\ W95,T &$ $&$ $&$ $&$0.554{-}0.792$&$0.512{-}0.732$&$ $&$0.541{-}0.774$ \\ \hline \noalign{\medskip} \noalign{\medskip} \hline\hline {\it apec} model & & & & SNIa & & &\\ \hline SNcc & W7 & W70 & WDD1 & WDD2 & WDD3 & CDD1 & CDD2 \\ \hline No06,S &$ $&$0.475{-}0.511$&$ $&$0.514{-}0.764$&$0.475{-}0.707$&$ $&$0.502{-}0.747$\\ No06,T &$ $&$ $&$ $&$0.564{-}0.789$&$0.526{-}0.735$&$ $&$0.553{-}0.773$\\ CL04,S &$ $&$ $&$0.591{-}0.886$&$0.502{-}0.759$&$0.581{-}0.701$&$0.608{-}0.841$&$0.490{-}0.741$\\ CL04,T &$ $&$ $&$0.647{-}0.855$&$0.561{-}0.787$&$0.523{-}0.734$&$0.663{-}0.799$&$0.549{-}0.771$\\ W95,S &$ $&$ $&$0.560{-}0.885$&$0.640{-}0.744$&$ $&$0.577{-}0.885$&$0.640{-}0.725$\\ W95,T &$ $&$ $&$0.598{-}0.895$&$0.561{-}0.763$&$ $&$0.615{-}0.868$&$0.561{-}0.745$\\ \hline \end{tabular} } \smallskip SNIa yields are computed from the full set of models for deflagration (W7, W70) and delayed detonation (WDDs, CDDs) scenarios by \citet{iwamoto99}. SNcc yields are integrated over a Salpeter ($x=1.35$) or a AY top-heavy ($x=0.95$) IMF, with abundance of the progenitor $Z=0.02$. Models for SNcc are taken from \citet[][No06]{nomoto06}, \citet[][CL04]{chieffi04} and \citet[][W95]{woosley95}. \end{table}