Type II supernovae from the Carnegie Supernova Project-I II. Physical parameter distributions from hydrodynamical modelling
Author
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Martínez, L.
Author
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Bersten, M. C.
Author
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Anderson, J. P.
Author
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Hamuy, M.
Author
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González Gaitán, S.
Author
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Forster Burón, Francisco
Author
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Orellana, M.
Author
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Stritzinger, M.
Author
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Phillips, M. M.
Author
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Gutiérrez, C. P.
Author
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Burns, C.
Author
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Contreras, C.
Author
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De Jaeger, T.
Author
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Ertini, K.
Author
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Folatelli, G.
Author
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Galbany, L.
Author
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Hoeflich, P.
Author
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Hsiao, E. Y.
Author
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Morrell, N.
Author
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Pessi, P. J.
Author
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Suntzeff, N. B.
Admission date
dc.date.accessioned
2022-07-25T15:48:07Z
Available date
dc.date.available
2022-07-25T15:48:07Z
Publication date
dc.date.issued
2022
Cita de ítem
dc.identifier.citation
A&A 660, A41 (2022)
es_ES
Identifier
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10.1051/0004-6361/202142076
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/186919
Abstract
dc.description.abstract
Linking supernovae to their progenitors is a powerful method for furthering our understanding of the physical origin of their observed differences
while at the same time testing stellar evolution theory. In this second study of a series of three papers where we characterise type II supernovae
(SNe II) to understand their diversity, we derive progenitor properties (initial and ejecta masses and radius), explosion energy, and 56Ni mass and its
degree of mixing within the ejecta for a large sample of SNe II. This dataset was obtained by the Carnegie Supernova Project-I and is characterised
by a high cadence of SNe II optical and near-infrared light curves and optical spectra that were homogeneously observed and processed. A large
grid of hydrodynamical models and a fitting procedure based on Markov chain Monte Carlo methods were used to fit the bolometric light curve
and the evolution of the photospheric velocity of 53 SNe II. We infer ejecta masses of between 7.9 and 14.8 M , explosion energies between 0.15
and 1.40 foe, and 56Ni masses between 0.006 and 0.069 M . We define a subset of 24 SNe (the ‘gold sample’) with well-sampled bolometric light
curves and expansion velocities for which we consider the results more robust. Most SNe II in the gold sample (∼88%) are found with ejecta
masses in the range of ∼8−10 M , coming from low zero-age main-sequence masses (9−12 M ). The modelling of the initial-mass distribution of
the gold sample gives an upper mass limit of 21.3+3.8
−0.4 M and a much steeper distribution than that for a Salpeter massive-star initial mass function
(IMF). This IMF incompatibility is due to the large number of low-mass progenitors found – when assuming standard stellar evolution. This may
imply that high-mass progenitors lose more mass during their lives than predicted. However, a deeper analysis of all stellar evolution assumptions
is required to test this hypothesis.
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Patrocinador
dc.description.sponsorship
National Science Foundation (NSF) AST-0306969
AST-0607438
AST-1008343
AST-1613426
AST-1613472
AST-1613455
Consejo Nacional de Investigaciones Cientificas y Tecnicas (CONICET)
UNRN PI2018 40B885
Hagler Institute of Advanced Study at Texas AM University
FCT under Project CRISP PTDC/FIS-AST-31546/2017
UIDB/00099/2020
Villum Fonden 28021
Independent Research Fund Denmark (IRFD) 8021-00170B
National Agency for Research and Development (ANID) AFB-170001
Ministry of Economy, Development, and Tourism's Millennium Science Initiative IC12009
Comision Nacional de Investigacion Cientifica y Tecnologica (CONICYT)
CONICYT FONDECYT 1200710
Spanish Government RYC2019-027683
Spanish MICIU project PID2020-115253GA-I00
National Science Foundation (NSF)
National Research Foundation of Korea AST-1715133
es_ES
Lenguage
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en
es_ES
Publisher
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EDP
es_ES
Type of license
dc.rights
Attribution-NonCommercial-NoDerivs 3.0 United States