1. ASASSN-15no: The Supernova that plays hide-and-seek
- Author
-
A. Morales-Garoffolo, Massimo Turatto, Leonardo Tartaglia, S. Taubenberger, G. Terreran, P. Ochner, Avet Harutyunyan, Maria Letizia Pumo, L. Tomasella, Enrico Cappellaro, Nancy Elias-Rosa, Luca Zampieri, S. Benetti, and A. Pastorello
- Subjects
Physics ,High Energy Astrophysical Phenomena (astro-ph.HE) ,010308 nuclear & particles physics ,Hide and seek ,Supernovae: general ,Library science ,FOS: Physical sciences ,Astronomy and Astrophysics ,01 natural sciences ,Supernovae: general, Supernovae: individual: ASASSN-15no, Astronomy and Astrophysics, Space and Planetary Science ,language.human_language ,Max planck institute ,German ,Astrophysics - Solar and Stellar Astrophysics ,Space and Planetary Science ,0103 physical sciences ,language ,Supernovae: individual: ASASSN-15no ,Astrophysics - High Energy Astrophysical Phenomena ,National laboratory ,010303 astronomy & astrophysics ,Solar and Stellar Astrophysics (astro-ph.SR) - Abstract
We report the results of our follow-up campaign of the peculiar supernova ASASSN-15no, based on optical data covering ~300 days of its evolution. Initially the spectra show a pure blackbody continuum. After few days, the HeI 5876 A transition appears with a P-Cygni profile and an expansion velocity of about 8700 km/s. Fifty days after maximum, the spectrum shows signs typically seen in interacting supernovae. A broad (FWHM~8000 km/s) Halpha becomes more prominent with time until ~150 days after maximum and quickly declines later on. At these phases Halpha starts to show an intermediate component, which together with the blue pseudo-continuum are clues that the ejecta begin to interact with the CSM. The spectra at the latest phases look very similar to the nebular spectra of stripped-envelope SNe. The early part (the first 40 days after maximum) of the bolometric curve, which peaks at a luminosity intermediate between normal and superluminous supernovae, is well reproduced by a model in which the energy budget is essentially coming from ejecta recombination and 56Ni decay. From the model we infer a mass of the ejecta Mej = 2.6 Msun; an initial radius of the photosphere R0 = 2.1 x 10^14 cm; and an explosion energy Eexpl = 0.8 x 10^51 erg. A possible scenario involves a massive and extended H-poor shell lost by the progenitor star a few years before explosion. The shell is hit, heated and accelerated by the supernova ejecta. The accelerated shell+ejecta rapidly dilutes, unveiling the unperturbed supernova spectrum below. The outer ejecta start to interact with a H-poor external CSM lost by the progenitor system about 9 -- 90 years before the explosion., Comment: 11 pages, 4 figures, in press to MNRAS
- Published
- 2018