Table 3
Input parameters for TARDIS model spectra.
Model | Luminosity | Time since explosion | Inner boundary | Outer boundary | Density | Composition |
log L [ L⊙] | texp (days) | vi (km s-1) | vo (km s-1) | |||
|
||||||
N5-3T | 9.10 | 19 | 7800 | 9400 | N5def | N5def |
N5-2T | 8.95 | 20 | 7800 | 9400 | N5def | N5def |
N5-2Tf | 8.95 | 20 | 8800 | 9400 | N5def | N5def |
N5-2Ts | 8.95 | 20 | 5800 | 9400 | N5def | N5def |
N5-2Th | 8.95 | 20 | 7800 | 9400 | N5def × 5 | N5def |
N5-2Tl | 8.95 | 20 | 7800 | 9400 | N5def × 0.2 | N5def |
N5-2Tlf | 8.95 | 20 | 8800 | 9400 | N5def × 0.2 | N5def |
N5-2Tls | 8.95 | 20 | 5800 | 9400 | N5def × 0.2 | N5def |
N5+2Tls | 8.85 | 24 | 5200 | 9400 | v> 5800 km s-1: N5def × 0.2 | N5def |
v< 5800 km s-1: N5def |
Notes. For the density and composition, we take a spherical average of velocity shells from the N5def model of Fink et al. (2014). The naming scheme of our models is defined as follows: N5-XT refers to TARDIS models (“T”) which are based on the N5def model from Fink et al. (2014), with “-X” referring to the phase of the spectrum. These times correspond to phases of −3 d, −2 d, and + 2 d relative to r-band maximum, assuming a rise time of ~22 (Phillips et al. 2007; Magee et al. 2016). The suffixes f/s refer to the photospheric velocity being fast/slow, while h/l refer to the ejecta density being higher/lower relative to the N5def model.
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