Free Access
| mekal model | SNIa | ||||||
| SNcc | W7 | W70 | WDD1 | WDD2 | WDD3 | CDD1 | CDD2 |
| 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 | ||||
apec model |
SNIa | ||||||
| SNcc | W7 | W70 | WDD1 | WDD2 | WDD3 | CDD1 | CDD2 |
| 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 |
,
obtained for different
theoretical SNe silicon-to-iron and nickel-to-iron ratios from the
observed Si/Fe and Ni/Fe ratios.
SNIa yields are computed from the
full set of models for deflagration (W7, W70) and delayed detonation
(WDDs, CDDs) scenarios by Iwamoto et al. (1999). 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 Nomoto et al. (2006, No06), Chieffi & Limongi (2004, CL04) and
Woosley & Weaver (1995, W95).
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