The delayed-detonation model of Type IA supernovae. 2: The detonation phase

1994 ◽  
Vol 427 ◽  
pp. 330 ◽  
Author(s):  
David Arnett ◽  
Eli Livne
2019 ◽  
Vol 490 (1) ◽  
pp. 578-599 ◽  
Author(s):  
Aleksandar Cikota ◽  
Ferdinando Patat ◽  
Lifan Wang ◽  
J Craig Wheeler ◽  
Mattia Bulla ◽  
...  

ABSTRACT Spectropolarimetry enables us to measure the geometry and chemical structure of the ejecta in supernova explosions, which is fundamental for the understanding of their explosion mechanism(s) and progenitor systems. We collected archival data of 35 Type Ia supernovae (SNe Ia), observed with Focal Reducer and Low-Dispersion Spectrograph (FORS) on the Very Large Telescope at 127 epochs in total. We examined the polarization of the Si ii λ6355 Å line ($p_{\rm Si\, \small {II}}$) as a function of time, which is seen to peak at a range of various polarization degrees and epochs relative to maximum brightness. We reproduced the $\Delta m_{15}\!-\!p_{\rm Si\, \small {II}}$ relationship identified in a previous study, and show that subluminous and transitional objects display polarization values below the $\Delta m_{15}\!-\!p_{\rm Si\, \small {II}}$ relationship for normal SNe Ia. We found a statistically significant linear relationship between the polarization of the Si ii λ6355 Å line before maximum brightness and the Si ii line velocity and suggest that this, along with the $\Delta m_{15}\!-\!p_{\rm Si\, \small {II}}$ relationship, may be explained in the context of a delayed-detonation model. In contrast, we compared our observations to numerical predictions in the $\Delta m_{15}\!-\!v_{\rm Si\, \small {II}}$ plane and found a dichotomy in the polarization properties between Chandrasekhar and sub-Chandrasekhar mass explosions, which supports the possibility of two distinct explosion mechanisms. A subsample of SNe displays evolution of loops in the q–u plane that suggests a more complex Si structure with depth. This insight, which could not be gleaned from total flux spectra, presents a new constraint on explosion models. Finally, we compared our statistical sample of the Si ii polarization to quantitative predictions of the polarization levels for the double-detonation, delayed-detonation, and violent-merger models.


2015 ◽  
Vol 92 (12) ◽  
Author(s):  
Ivo R. Seitenzahl ◽  
Matthias Herzog ◽  
Ashley J. Ruiter ◽  
Kai Marquardt ◽  
Sebastian T. Ohlmann ◽  
...  

2009 ◽  
Vol 693 (2) ◽  
pp. 1188-1208 ◽  
Author(s):  
Casey A. Meakin ◽  
Ivo Seitenzahl ◽  
Dean Townsley ◽  
George C. Jordan ◽  
James Truran ◽  
...  

2005 ◽  
Vol 623 (1) ◽  
pp. 337-346 ◽  
Author(s):  
Vadim N. Gamezo ◽  
Alexei M. Khokhlov ◽  
Elaine S. Oran

2020 ◽  
Vol 499 (4) ◽  
pp. 4725-4747
Author(s):  
Doron Kushnir ◽  
Nahliel Wygoda ◽  
Amir Sharon

ABSTRACT Type Ia supernovae (SNe Ia) are likely the thermonuclear explosions of carbon–oxygen (CO) white-dwarf (WD) stars, but their progenitor systems remain elusive. Recent studies have suggested that a propagating detonation within a thin helium shell surrounding a sub-Chandrasekhar mass CO core can subsequently trigger a detonation within the core (the double-detonation model, DDM). The outcome of this explosion is similar to a central ignition of a sub-Chandrasekhar mass CO WD (SCD). While SCD is consistent with some observational properties of SNe Ia, several computational challenges prohibit a robust comparison to the observations. We focus on the observed t0−MNi56 relation, where t0 (the γ-rays’ escape time from the ejecta) is positively correlated with MNi56 (the synthesized 56Ni mass). We apply our recently developed numerical scheme to calculate SCD and show that the calculated t0−MNi56 relation, which does not require radiation transfer calculations, converges to an accuracy of a few per cent. We find a clear tension between our calculations and the observed t0−MNi56 relation. SCD predicts an anticorrelation between t0 and MNi56, with $t_0\approx 30\, \textrm{d}$ for luminous ($M_\text{Ni56}\gtrsim 0.5\, \mathrm{ M}_{\odot }$) SNe Ia, while the observed t0 is in the range of $35\!-\!45\, \textrm{d}$. We show that this tension is larger than the uncertainty of the results, and that it exists in all previous studies of the problem. Our results hint that more complicated models are required, but we argue that DDM is unlikely to resolve the tension with the observations.


2012 ◽  
Vol 759 (1) ◽  
pp. 53 ◽  
Author(s):  
G. C. Jordan ◽  
C. Graziani ◽  
R. T. Fisher ◽  
D. M. Townsley ◽  
C. Meakin ◽  
...  

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