P. Hoflich et al., DELAYED DETONATION MODELS FOR NORMAL AND SUBLUMINOUS TYPE IA SUPERNOVAE - ABSOLUTE BRIGHTNESS, LIGHT CURVES, AND MOLECULE FORMATION, The Astrophysical journal, 444(2), 1995, pp. 831-847
We compute optical and infrared light curves of the pulsating class of
delayed detonation models for Type Ia supernovae (SN Ia's) using an e
laborate treatment of the LTE radiation transport, equation of state a
nd ionization balance, expansion opacity including the cooling by CO,
CO+, and SiO, and a Monte Carlo gamma-ray deposition scheme. The model
s have an amount of Ni-56 in, the range from similar or equal to 0.1 M
. up to 0.7 M. depending on the density at which the transition from a
deflagration to a detonation occurs. Models with a large nickel produ
ction give light curves comparable to those of typical Type Ia superno
vae. Subluminous supernovae can be explained by models with a low nick
el production. Multiband light curves are presented in comparison with
the normally bright event SN 1992bc and the subluminous events SN 199
1bg and SN 1992bo to establish the principle that the delayed detonati
on paradigm in Chandrasekhar mass models may give a common explosion m
echanism accounting for both normal and subluminous SN Ia's. Secondary
IR-maxima are formed in the models of normal SN Ia's as a photospheri
c effect if the photospheric radius continues to increase well after m
aximum light. Secondary maxima appear later and stronger in models wit
h moderate expansion velocities and with radioactive material closer t
o the surface. Model light curves for subluminous SN Ia's tend to show
only one ''late'' IR-maximum. In some delayed detonation models shell
-like envelopes form, which consist of unburned carbon and oxygen. The
formation of molecules in these envelopes is addressed. If the model
retains a C/O-envelope and is subluminous, strong vibration bands of C
O may appear, typically several weeks past maximum light. CO should be
very weak or absent in normal SN Ia's.