The failure of prompt explosion Delayed explosion or
- Slides: 34
The failure of prompt explosion. Delayed explosion, or how to revive a stalled shock wave?
1 -D spherically symmetric collapse let’s see the “movie” H. -T. Janka, K. Langanke, A. Marek, G. Martnez-Pinedo and B. Muller Phys. Rept. 442 (2007) 38
The properties of the Neutrino flux Cumulative neutrino “light” curve (based on Nadyozhin 1978) Nonthermal e
Liebendoerfer et al. 2003 Solid lines: 40 MSun progenetor dashed: 13 MSun progenetor
The spectral properties of the Neutrino flux Total energy radiated. Characteristic time. Neutrino individual energies (ε). Neutrino flavors.
Neutrino spectra for thermal phase Energy spectra. Fermi−Dirac law: High-energy cutoff (relevant to ):
Core-collapse SNe (all other Types but Ia) The SN outburst is triggered by the gravitational collapse of the “iron” core of a mass MFe=(1. 2 2) M into a neutron star. About (10 15)% MFec 2 is radiated in the form of neutrinos and antineutrinos of all the flavors (e, , ): The explosion energy (kinetic energy of the envelope expansion): Eexp = (0. 5 2) 1051 erg it comes from the shock wave created at the boundary between a new-born neutron star and the envelope to be expelled. Rich nucleosynthesis — from neutrino-induced creation of light element in C-O and He shells through synthesis of heavy nuclides by neutron capture at the bottom of expelled envelope
Delayed explosion Wilson J R (1985) Numerical Astrophysics (Boston: Jones and Barlett)
The mechanism of the core-collapse SNe is still under detailed study Spherically-symmetrical collapse. An empirical theorem: Spherically-symmetrical models do not result in expulsion of an envelope; the SN outburst does not occur: the envelope falls back on the collapsed core. Corollary: One has to address to 2 - and, perhaps, 3 -dimensional models to convert the stalled accreting shock into an outgoing blast wave.
Neutrino-convective mechanism of supernova explosion
Convective instability criterion A Chemically uniform medium is convectively unstable, if > A For non-uniform media > A +
NEUTRINO-CONVECTIVE MECHANISM 150 и 300 ms after bounce Liebendoerfer (2011) Convective instability condition 10^4
Dynamics of gravitational collapse Expulsion of supernova envelope (how? ) neutrinosphere
Janka (2001)
3 -D simulations:
J. M. Blondin, A. Mezzacappa “Pulsar spins from an instability in the accretion shock of SN”
From astrophysical complexity to the simplicity of a water fountain Foglizzo et al 2018
O’Connor E, Couch S. (2015) A. Marek and H. -T. Janka
Schematic Supernova «light curves»
The failure of prompt explosion. Delayed explosion, or how to revive a stalled shock wave? SN 1987 A – the only supernova with neutrino signal detected Janka et al, Prog. Theor. Exp. Phys. (2012)
SN 1987 A – the only supernova with neutrino signal detected
SN 1987 А Image from skyandtelescope. com
Small Magellanic Cloud Milky Way Large Magellanic Cloud SN 1987 A Southern Cross 23. 02. 1987 Cerro Tollolo Inter-american Observatory, Chile
The star that exploded on February 23 in the Large Magellanic Cloud (the progenitor of supernova 1987 A) has now been identified. It was catalogued by in 1969 as an OB star of 12 th magnitude and given the designation Sanduleak-69 202. Observations at the European Southern Observatory in the mid-1970's allowed to classify it as of spectral type B 3 I, that is a very hot, supergiant star. Credit: ESO
SN 1987 A ring evolution
Signals from SN 1987 A on 23 Feb. 1987: Kamioka All three detectors saw a cluster of events at ~7: 35 UT Baksan q 330 tons liquid scint q threshold ~10 Me. V q 5 events in 9. 1 sec. q q IMB water Cerenkov 5000 tons fiducial threshold 20 Me. V 8 events in 6 seconds q q water Cerenkov 2140 tons fiducial threshold ~6 Me. V 12 events in 12. 4 sec.
Baksan Underground Scintillation Telescope 31
+4 mv Mc. Naught SN 1987 А Shelton +6 Discovery Jones +8 Mont Blanc Kamioka, IMB, Baksan Sk – 69 o 202 +10 Radio (21 cм) Shelton +12 Feb 23 Feb 24 Feb 25 0 h 2 h 52 m 7 h 36 m 9 h 22 m 15 h 54 m
Detection efficiency Kotake et al (2006)
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