Abstract:Knowledge of the progenitors of core-collapse supernovae is a fundamental component in understanding the explosions. The recent progress in finding such stars is reviewed. The minimum initial mass that can produce a supernova has converged to 8 ± 1M⊙, from direct detections of red supergiant progenitors of II-P SNe and the most massive white dwarf progenitors, although this value is model dependent. It appears that most type Ibc supernovae arise from moderate mass interacting binaries. The highly energetic, br… Show more
“…Two of the nearest events, SN1987A and SN1993J, which have fairly massive and wellobserved progenitors, are both peculiar. Aside from these two outliers, the rest of the supernovae that have thus far had their progenitors observed on archival images of the host galaxy, or upper limits placed on their luminosity, are SN IIP whose progenitors are mostly RSGs with inferred masses clustering around the low end of the progenitor ZAMS mass range for which core collapse is a possible evolutionary outcome, M 8 1 ZAMS » M (Smartt 2009;Fraser et al 2011). However, there are several events with progenitors having inferred M 12 ZAMS » -25 M within the range of progenitors used in our simulations.…”
Section: Observational Samplementioning
confidence: 99%
“…This requires corrections for estimated mass loss during progenitor evolution and a compact remnant mass estimate. Since this method requires high-quality photometric and spectroscopic data, it has only been applied to a handful of events where such data are available (e.g., Zampieri et al 2003;Baklanov et al 2005;Utrobin 2007;Utrobin & Chugai 2008, 2009Pastorello et al 2009;Dall'Ora et al 2014). Typically, these models of explosions in RSGs predict significantly higher ZAMS masses than those obtained by direct imaging.…”
We present four ab initio axisymmetric core-collapse supernova simulations initiated from 12, 15, 20, and 25 M zero-age main sequence progenitors. All of the simulations yield explosions and havebeen evolved for at least 1.2 s after core bounce and 1 s after material first becomes unbound. These simulations were computed with our CHIMERA code employing RbR spectral neutrino transport, special and general relativistic transport effects, and state-of-the-art neutrino interactions. Continuing the evolution beyond 1 s after core bounce allows the explosions to develop more fully and the processes involved in powering the explosions to become more clearly evident. We compute explosion energy estimates, including the negative gravitational binding energy of the stellar envelope outside the expanding shock, of 0.34, 0.88, 0.38, and 0.70 Bethe (B≡10 51 erg) and increasing at 0.03, 0.15, 0.19, and 0.52 B s 1 -, respectively, for the 12, 15, 20, and 25 M models at the endpoint of this report. We examine the growth of the explosion energy in our models through detailed analyses of the energy sources and flows. We discuss how the explosion energies may be subject to stochastic variations as exemplfied by the effect of the explosion geometry of the 20 M model in reducing its explosion energy. We compute the proto-neutron star masses and kick velocities. We compare our results for the explosion energies and ejected Ni 56 masses against some observational standards despite the large error bars in both models and observations.
“…Two of the nearest events, SN1987A and SN1993J, which have fairly massive and wellobserved progenitors, are both peculiar. Aside from these two outliers, the rest of the supernovae that have thus far had their progenitors observed on archival images of the host galaxy, or upper limits placed on their luminosity, are SN IIP whose progenitors are mostly RSGs with inferred masses clustering around the low end of the progenitor ZAMS mass range for which core collapse is a possible evolutionary outcome, M 8 1 ZAMS » M (Smartt 2009;Fraser et al 2011). However, there are several events with progenitors having inferred M 12 ZAMS » -25 M within the range of progenitors used in our simulations.…”
Section: Observational Samplementioning
confidence: 99%
“…This requires corrections for estimated mass loss during progenitor evolution and a compact remnant mass estimate. Since this method requires high-quality photometric and spectroscopic data, it has only been applied to a handful of events where such data are available (e.g., Zampieri et al 2003;Baklanov et al 2005;Utrobin 2007;Utrobin & Chugai 2008, 2009Pastorello et al 2009;Dall'Ora et al 2014). Typically, these models of explosions in RSGs predict significantly higher ZAMS masses than those obtained by direct imaging.…”
We present four ab initio axisymmetric core-collapse supernova simulations initiated from 12, 15, 20, and 25 M zero-age main sequence progenitors. All of the simulations yield explosions and havebeen evolved for at least 1.2 s after core bounce and 1 s after material first becomes unbound. These simulations were computed with our CHIMERA code employing RbR spectral neutrino transport, special and general relativistic transport effects, and state-of-the-art neutrino interactions. Continuing the evolution beyond 1 s after core bounce allows the explosions to develop more fully and the processes involved in powering the explosions to become more clearly evident. We compute explosion energy estimates, including the negative gravitational binding energy of the stellar envelope outside the expanding shock, of 0.34, 0.88, 0.38, and 0.70 Bethe (B≡10 51 erg) and increasing at 0.03, 0.15, 0.19, and 0.52 B s 1 -, respectively, for the 12, 15, 20, and 25 M models at the endpoint of this report. We examine the growth of the explosion energy in our models through detailed analyses of the energy sources and flows. We discuss how the explosion energies may be subject to stochastic variations as exemplfied by the effect of the explosion geometry of the 20 M model in reducing its explosion energy. We compute the proto-neutron star masses and kick velocities. We compare our results for the explosion energies and ejected Ni 56 masses against some observational standards despite the large error bars in both models and observations.
“…Fortunately, κ is a parameter that characterizes the microphysics of the ejecta and therefore can be calculated in first principles based on our knowledge about the ejecta composition. It is believed that the progenitor of an SN Ic (broad-lined or not) is a massive single star or a low-mass star in a binary (Smartt 2009). The ejecta of such a star explosion are mainly composed of 16 O, 20 Ne and 24 Mg (Iwamoto et al 2000;Nakamura et al 2001a;Maeda et al 2002).…”
Broad-lined type Ic supernovae (SNe Ic-BL) are peculiar stellar explosions that distinguish themselves from ordinary SNe. Some SNe Ic-BL are associated with long-duration ( 2 s) gamma-ray bursts (GRBs). Black holes and magnetars are two types of compact objects that are hypothesized to be central engines of GRBs. In spite of decades of investigations, no direct evidence for the formation of black holes or magnetars has been found for GRBs so far. Here we report the finding that the early peak (t 50 days) and late-time (t 300 days) slow decay displayed in the light curves of both SNe 1998bw (associated with GRB 980425) and 2002ap (not GRB-associated) can be attributed to magnetar spin-down with initial rotation period P 0 ∼ 20 ms, while the intermediate-time (50 t 300 days) exponential decline is caused by radioactive decay of 56 Ni. The connection between the early peak and late-time slow decline in the light curves is unexpected in alternative models. We thus suggest that GRB 980425 and SN 2002ap were powered by magnetars.
“…Core-Collapse (CC) SNe, whose progenitors are thought to be young massive stars (e.g. Turatto 2003;Smartt 2009;Anderson et al 2012), are observationally classified in three major classes, according to the strength of lines in optical spectra (e.g. Filippenko 1997): Type II SNe show hydrogen lines in their spectra, while Types Ib and Ic do not, with Type Ib SNe showing helium and Type Ic SNe showing neither hydrogen nor helium.…”
We present an analysis of the relative frequencies of different supernova (SN) types in spirals with various morphologies and in barred or unbarred galaxies. We use a well-defined and homogeneous sample of spiral host galaxies of 692 SNe from the Sloan Digital Sky Survey in different stages of galaxy-galaxy interaction and activity classes of nucleus. We propose that the underlying mechanisms shaping the number ratios of SNe types can be interpreted within the framework of interaction-induced star formation, in addition to the known relations between morphologies and stellar populations. We find a strong trend in behaviour of the N Ia /N CC ratio depending on host morphology, such that early spirals include more Type Ia SNe. The N Ibc /N II ratio is higher in a broad bin of early-type hosts. The N Ia /N CC ratio is nearly constant when changing from normal, perturbed to interacting galaxies, then declines in merging galaxies, whereas it jumps to the highest value in post-merging/remnant galaxies. In contrast, the N Ibc /N II ratio jumps to the highest value in merging galaxies and slightly declines in post-merging/remnant subsample. The interpretation is that the star formation rates and morphologies of galaxies, which are strongly affected in the final stages of interaction, have an impact on the number ratios of SNe types. The N Ia /N CC (N Ibc /N II ) ratio increases (decreases) from star-forming to active galactic nuclei (AGN) classes of galaxies. These variations are consistent with the scenario of an interaction-triggered starburst evolving into AGN during the later stages of interaction, accompanied with the change of star formation and transformation of the galaxy morphology into an earlier type.
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