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Table 3

Properties of the SN modelling.

Simple power-law + free host magnitude
α1 = 0.69 ± 0.02

Band Host magnitude Luminosity Stretch χ2/ d.o.f.
(mag) factor k factor s

g 24.65 ± 0.12 0.86 ± 0.03 0.94 ± 0.02 194.9 / 146
r 24.06 ± 0.04 1.25 ± 0.02 0.89 ± 0.02
i 24.17 ± 0.08 1.10 ± 0.01 0.92 ± 0.01
z 24.31 ± 0.12 0.99 ± 0.02 0.92 ± 0.03
J 24.22 ± 0.22 1.12 ± 0.09 0.74 ± 0.12
H ... ... ...

Smoothly broken power-law + fixed host magnitude
α1 = 0.67 ± 0.02, α2 = 2.00 (fixed), tb (days) = 9.7 ± 4.4,
n = 10 (fixed)

Band Host magnitude Luminosity Stretch χ2/ d.o.f.
(mag) factor k factor s

g 24.62 0.88 ± 0.05 0.97 ± 0.02 186.6 / 150
r 24.09 1.25 ± 0.02 0.90 ± 0.01
i 24.09 1.11 ± 0.02 0.92 ± 0.01
z 24.15 0.99 ± 0.03 0.92 ± 0.03
J 23.96 1.06 ± 0.09 0.68 ± 0.09
H 23.84 ... ...

Notes. Best-fit parameters of the grizJH band light curve fits. We modelled grizJ light curves with a SN1998bw template redshifted to z = 0.2825, as described in Zeh et al. (2004), which is superposed on a simple power-law or smoothly broken power-law (Beuermann et al. 1999), where α denotes the decay slope, tb the break time, and n the smoothness, to account for the early emission and the flux from the host galaxy at the explosion site. For the H band, we used the afterglow models only. We assumed that the afterglow component evolves achromatically from the g to the H band. The supernova and afterglow light curve is equally well fitted with the two models. Column 2 gives the contribution of the host galaxy in the used aperture. See Sect. 3.3.2 for details.

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