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Table 21

CSI Parameters for the full CSP SN IIn Sample.

SN L(Hαbroad) v s v w w n H t sh
(1040 erg s-1) (103 km s-1) (102 km s-1) (103 km s-1) (10-3 M yr-1) (1015 g cm-1) (108 cm-3) (1015 cm) (1015 cm) (1015 cm) (yr before core collapse)

05ip 4 1.0 1.2 16.0 0.2−0.4 1.0−2.0 >3×10-3 <0.1 >325.1
05kj 1.0−3.4 3.0 6.0 3.0 1.4−4.8 1.5−5.0 >1.8 <0.4 >4.4
06aa 1.1−3.4 2.0 6.0 2.5 5.0−16.0 5.7−17.1 >7.6 <0.5 >1.8 1.3 0.7
06bo <0.6−0.9 >1.0 6.0 2.5 <23.0−34.0 <24.0−36.0 >3.8 <0.2–0.9 >1.5−2.4
06jd 3.0−13.0 1.6 <1.6 16.0 <7.0−32.0 29.3−126.9 >10-2 <3.0 >213.1 55.3 >110
06qq 5.6−12.1 6.0 <2.0 10.0 <0.3−0.7 1.0−2.2 >11.4 <2.5 >7.9 6.6 >10
08fq 15.0 7.5 5.0 9.0 1.1 1.4 >9.0 <0.8 >6.1 3.5 0.5−0.0 / >3.9−2.2

Notes.Luminosity values for Hα of SNe 2005ip and 2006jd are from S12 (here, we use the intermediate component, which is associated with post-shock gas). vs, vw, , and nH for SNe 2005ip and 2006jd are from Smith et al. (2009b) and S12, respectively. The mass-loss rate and the wind density (w) of SN 2005ip are from Smith et al. (2009b). The limits for and of SNe 2005ip and 2006jd are obtained from the first and the last spectral epochs (Smith et al. 2009b, S12), and from the assumed . The CSM of SN 2006jd is characterized by the presence of a dense structure, as indicated by the re-brightening of the r-band light curve approximately 400 days after explosion. Its radius () and epoch of the outburst are computed from the epoch of the r-band maximum and from the assumed and vw. In the case of SN 2008fq, we present the epochs of two outbursts that formed the inner and the outer CSM, as described in Sect. 6. Here, is the extent of the inner CSM, the inner radius of the outer CSM, and the outer radius of the outer CSM.

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