Evidence for sub - Chandrasekhar- mass progenitors of type Ia supernovae at the faint end of the width luminosity relation
Author
dc.contributor.author
Blondin, Stephane
Author
dc.contributor.author
Dessart, Luc
Author
dc.contributor.author
Hillier, D. John
Author
dc.contributor.author
Khokhlov, Alexei M.
Admission date
dc.date.accessioned
2018-06-20T14:27:48Z
Available date
dc.date.available
2018-06-20T14:27:48Z
Publication date
dc.date.issued
2017
Cita de ítem
dc.identifier.citation
Monthly Notices of The Royal Astronomical Society Vol. 470 ( 1): 157-165
es_ES
Identifier
dc.identifier.other
10.1093/mnras/stw2492
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/149064
Abstract
dc.description.abstract
The faster light-curve evolution of low-luminosity Type Ia supernovae (SNe Ia) suggests that they could result from the explosion of white dwarf (WD) progenitors below the Chandrasekhar mass (M-Ch). Here we present 1D non-local thermodynamic equilibrium time-dependent radiative transfer simulations of pure central detonations of carbon-oxygen WDs with a mass (M-tot) between 0.88 and 1.15 M-circle dot and a Ni-56 yield between 0.08 and 0.84 M-circle dot. Their lower ejecta density compared to M-Ch models results in a more rapid increase of the luminosity at early times and an enhanced gamma-ray escape fraction past maximum light. Consequently, their bolometric light curves display shorter rise times and larger post-maximum decline rates. Moreover, the higher M(Ni-56)/M-tot ratio at a given Ni-56 mass enhances the temperature and ionization level in the spectrum-formation region for the less luminous models, giving rise to bluer colours at maximum light and a faster post-maximum evolution of the B - V colour. For sub-M-Ch models fainter than M-B approximate to -18.5 mag at peak, the greater bolometric decline and faster colour evolution lead to a larger B-band post-maximum decline rate, Delta M-15(B). In particular, all of our previously published M-Ch models (standard and pulsational delayed detonations) are confined to Delta M-15(B) < 1.4 mag, while the sub-M-Ch models with M-tot less than or similar to 1 M-circle dot extend beyond this limit to Delta M-15(B) approximate to 1.65 mag for a peak M-B approximate to -17 mag, in better agreement with the observed width-luminosity relation (WLR). Regardless of the precise ignition mechanism, these simulations suggest that fast-declining SNe Ia at the faint end of the WLR could result from the explosion of WDs whose mass is significantly below the Chandrasekhar limit.
es_ES
Patrocinador
dc.description.sponsorship
Programme National de Physique Stellaire (PNPS) of CNRS/INSU, France
STScI
HST-AR-12640.01
NASA
NNX14AB41G