ASASSN-15no: the Supernova that plays hide-and-seek

Abstract We report the results of our follow-up campaign of the peculiar supernova ASASSN-15no, based on optical data covering ∼300 d of its evolution. Initially the spectra show a pure blackbody continuum. After few days, the HeI λλ 5876 transition appears with a P-Cygni profile and an expansion ve...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2018-05, Vol.476 (1), p.261-270
Hauptverfasser: Benetti, S, Zampieri, L, Pastorello, A, Cappellaro, E, Pumo, M L, Elias-Rosa, N, Ochner, P, Terreran, G, Tomasella, L, Taubenberger, S, Turatto, M, Morales-Garoffolo, A, Harutyunyan, A, Tartaglia, L
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Sprache:eng
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Zusammenfassung:Abstract We report the results of our follow-up campaign of the peculiar supernova ASASSN-15no, based on optical data covering ∼300 d of its evolution. Initially the spectra show a pure blackbody continuum. After few days, the HeI λλ 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 ∼ 8000 km s−1)  Hα  becomes more prominent with time until ∼150  d after maximum and quickly declines later on. At these phases  Hαstarts 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 56Ni decay. From the model, we infer a mass of the ejecta Mej = 2.6 M⊙; an initial radius of the photosphere R0 = 2.1 × 1014 cm; and an explosion energy Eexpl = 0.8 × 1051 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.
ISSN:0035-8711
1365-2966
DOI:10.1093/mnras/sty166