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The light curves of Type Ia supernovae (SNe Ia) are powered by the radioactive decay of 56 Ni to 56 Co at early times, and the decay of 56 Co to 56 Fe from 60 d after explosion. We examine the evolution of the [Co III] 5893 emission complex during the nebular phase for SNe Ia with multiple nebular spectra and show that the line flux follows the square of the mass of 56 Co as a function of time. This result indicates both efficient local energy deposition from positrons produced in 56 Co decay and long-term stability of the ionization state of the nebula. We compile SN Ia nebular spectra from the literature and present 21 new late-phase spectra of 7 SNe Ia, including SN 2014J. From these we measure the flux in the [Co III] 5893 line and remove its well-behaved time dependence to infer the initial mass of 56 Ni (M Ni ) produced in the explosion. We then examine 56 Ni yields for different SN Ia ejected masses (M ej -calculated using the relation between light-curve width and ejected mass) and find that the 56 Ni masses of SNe Ia fall into two regimes: for narrow light curves (low stretch s 0.7-0.9), M Ni is clustered near M Ni 0.4 M and shows a shallow increase as M ej increases from 1 to 1.4 M ; at high stretch, M ej clusters at the Chandrasekhar mass (1.4 M ) while M Ni spans a broad range from 0.6 to 1.2 M . This could constitute evidence for two distinct SN Ia explosion mechanisms.
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Childress et al. (2015) studied this question.
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