Journal
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 476, Issue 1, Pages 261-270Publisher
OXFORD UNIV PRESS
DOI: 10.1093/mnras/sty166
Keywords
supernovae: general; supernovae: individual: ASASSN-15no
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Funding
- PRIN-INAF (project 'Transient Universe: unveiling new types of stellar explosions with PESSTO')
- German Research Foundation (DFG) [TRR 33]
- Alfred P. Sloan Foundation
- National Science Foundation
- U.S. Department of Energy Office of Science
- University of Arizona
- Brazilian Participation Group
- Brookhaven National Laboratory
- Carnegie Mellon University
- University of Florida
- French Participation Group
- German Participation Group
- Harvard University
- Instituto de Astrofisica de Canarias
- Michigan State/Notre Dame/JINA Participation Group
- Johns Hopkins University
- Lawrence Berkeley National Laboratory
- Max Planck Institute for Astrophysics
- Max Planck Institute for Extraterrestrial Physics
- New Mexico State University
- New York University
- Ohio State University
- Pennsylvania State University
- University of Portsmouth
- Princeton University
- Spanish Participation Group
- University of Tokyo
- University of Utah
- Vanderbilt University
- University of Virginia
- University of Washington
- Yale University
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We report the results of our follow-up campaign of the peculiar supernova ASASSN-15no, based on optical data covering similar to 300 d of its evolution. Initially the spectra show a pure black-body continuum. After few days, the HeI lambda lambda 5876 transition appears with a P-Cygni profile and an expansion velocity of about 8700 km s(-1). Fifty days after maximum, the spectrum shows signs typically seen in interacting supernovae. A broad (FWHM similar to 8000 km s(-1)) H alpha becomes more prominent with time until similar to 150 d after maximum and quickly declines later on. At these phases Hastarts to show an intermediate component, which together with the blue pseudo-continuum are clues that the ejecta begin to interact with the circumstellar medium (CSM). The spectra at the latest phases look very similar to the nebular spectra of stripped-envelope SNe. The early part (the first 40 d 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 Ni-56 decay. From the model, we infer a mass of the ejecta M-ej = 2.6M(circle dot); an initial radius of the photosphere R-0 = 2.1 x 10(14) cm; and an explosion energy E-expl = 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 yr before the explosion.
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