The Peculiar Type II Supernova 1997D: A Case for a Very Low [TSUP]56[/TSUP]N[CLC]i[/CLC] Mass
Author(s) -
M. Turatto,
P. A. Mazzali,
Timothy R. Young,
K. Nomoto,
K. Iwamoto,
S. Benetti,
E. Cappellaro,
I. J. Danziger,
D. F. De Mello,
M. M. Phillips,
N. B. Suntzeff,
A. Clocchiatti,
A. Piemonte,
B. Leibundgut,
R. Covarrubias,
J. Maza,
J. Sollerman
Publication year - 1998
Publication title -
the astrophysical journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.376
H-Index - 489
eISSN - 1538-4357
pISSN - 0004-637X
DOI - 10.1086/311324
Subject(s) - physics , astrophysics , supernova , light curve , radius , luminosity , spectral line , solar mass , ejecta , brightness , line (geometry) , astronomy , stars , galaxy , geometry , computer security , mathematics , computer science
Artículo de publicación ISISN 1997D in NGC 1536 is possibly the least luminous and energetic Type II supernova discovered to date. The entire light curve is subluminous, never reaching M-v = -14.65. The radioactive tail follows the Co-56 decay slope. In the case of a nearly complete trapping of the gamma-rays, the Ni-56 mass derived from the tail brightness is extremely small, similar to 0.002 M.. At discovery, the spectra showed a red continuum and line velocities on the order of 1000 km s(-1). The luminosity and the photospheric expansion velocity suggest that the explosion occurred about 50 days before discovery and that a plateau probably followed. Model light curves and spectra of the explosion of a 26 M. star successfully fitted the observations. Low-mass models are inconsistent with the observations. The radius of the progenitor, constrained by the prediscovery upper limits, is R-0 less than or similar to 300 R.. A low explosion energy of similar to 4 x 10(50) ergs is then required in the modeling. The strong Pa II lines in the photospheric spectra are reproduced with a solar abundance and low T-eff. A scenario in which the low Ni-56 mass observed in SN 1997D is due to fallback of material onto the collapsed remnant of the explosion of a 25-40 M. star appears to be favored over the case of the explosion of an 8-10 M. star with low Ni-56 production
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