2011
DOI: 10.1111/j.1365-2966.2011.17229.x
|View full text |Cite
|
Sign up to set email alerts
|

Observed fractions of core-collapse supernova types and initial masses of their single and binary progenitor stars

Abstract: We analyse the observed fractions of core-collapse supernova (SN) types from the Lick Observatory Supernova Search (LOSS), and we discuss the corresponding implications for massive star evolution. For a standard initial mass function, observed fractions of SN types cannot be reconciled with the expectations of single-star evolution. The mass range of Wolf-Rayet (WR) stars that shed their hydrogen envelopes via their own mass-loss accounts for less than half of the observed fraction of Type Ibc supernovae (SNe … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

35
522
2
3

Year Published

2011
2011
2016
2016

Publication Types

Select...
6
3
1

Relationship

2
8

Authors

Journals

citations
Cited by 508 publications
(562 citation statements)
references
References 159 publications
(346 reference statements)
35
522
2
3
Order By: Relevance
“…The latter prescription is under the assumption that the BH formation is controlled by the compactness of the stellar core at the time of collapse: low compactness stars are more likely to explode as SNe and produce NSs, while high-compactness stars are more likely to evolve to failed SNe that produce BHs (O'Connor & Ott 2011). In this case we assume MBH = MHe or MCO, where MHe is the He core masses prior to core collapse (e.g., Smith et al 2011;Smith & Arnett 2014;Shiode & Quataert 2014;Sukhbold & Woosley 2014;Clausen et al 2015;Kochanek 2014Kochanek , 2015. The value of MHe is determined as follows (Hurley et al 2000, for a detailed description).…”
Section: Remnant Massmentioning
confidence: 99%
“…The latter prescription is under the assumption that the BH formation is controlled by the compactness of the stellar core at the time of collapse: low compactness stars are more likely to explode as SNe and produce NSs, while high-compactness stars are more likely to evolve to failed SNe that produce BHs (O'Connor & Ott 2011). In this case we assume MBH = MHe or MCO, where MHe is the He core masses prior to core collapse (e.g., Smith et al 2011;Smith & Arnett 2014;Shiode & Quataert 2014;Sukhbold & Woosley 2014;Clausen et al 2015;Kochanek 2014Kochanek , 2015. The value of MHe is determined as follows (Hurley et al 2000, for a detailed description).…”
Section: Remnant Massmentioning
confidence: 99%
“…(e.g. Bressan et al 2002;Eldridge, Izzard & Tout 2008;Eldridge, Langer & Tout 2011;Smith et al 2011). To qualitatively examine the relationship between this ratio and metallicity, we use the extracted global galaxy metallicities 8 available for only 196 CC SNe hosts from the SDSS DR10.…”
Section: Dependence Of Relative Frequencies Of Sne Types On Host Morpmentioning
confidence: 99%
“…While the close-binary evolution scenario offers an attractive solution to both core-collapse SN statistics (see, e.g., Podsiadlowski et al 1992;Eldridge et al 2008;Smith et al 2011) and inferred ejecta properties (Ensman & Woosley 1988;Woosley et al 1995), it is not clear today what fraction arises from the explosion of stars that evolve in isolation. The diversity of massive close binaries can qualitatively explain the observed diversity of SNe IIb (Claeys et al 2011), but for moderate main-sequence masses, the binary channel seems to favour the production of SNe ‹ email: Luc.Dessart@oca.eu Ib (Yoon et al 2010).…”
Section: Introductionmentioning
confidence: 99%