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 g′r′i′z′JH band light curve fits. We modelled g′r′i′z′J 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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