2013ApJ...776...97M


Query : 2013ApJ...776...97M

2013ApJ...776...97M - Astrophys. J., 776, 97 (2013/October-3)

The effects of curvature and expansion on helium detonations on white dwarf surfaces.

MOORE K., TOWNSLEY D.M. and BILDSTEN L.

Abstract (from CDS):

Accreted helium layers on white dwarfs have been highlighted for many decades as a possible site for a detonation triggered by a thermonuclear runaway. In this paper, we find the minimum helium layer thickness that will sustain a steady laterally propagating detonation and show that it depends on the density and composition of the helium layer, specifically 12C and 16O. Detonations in these thin helium layers have speeds slower than the Chapman-Jouget (CJ) speed from complete helium burning, vCJ= 1.5x109 cm/s. Though gravitationally unbound, the ashes still have unburned helium (~80% in the thinnest cases) and only reach up to heavy elements such as 40Ca, 44Ti, 48Cr, and 52Fe. It is rare for these thin shells to generate large amounts of 56Ni. We also find a new set of solutions that can propagate in even thinner helium layers when 16O is present at a minimum mass fraction of ~0.07. Driven by energy release from α captures on 16O and subsequent elements, these slow detonations only create ashes up to 28Si in the outer detonated He shell. We close by discussing how the unbound helium burning ashes may create faint and fast "Ia" supernovae as well as events with virtually no radioactivity, and speculate on how the slower helium detonation velocities impact the off-center ignition of a carbon detonation that could cause a Type Ia supernova in the double detonation scenario.

Abstract Copyright: ∼

Journal keyword(s): binaries: close - nuclear reactions, nucleosynthesis, abundances - shock waves - supernovae: general - white dwarfs

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* S And No* 00 42 43.12368 +41 16 03.2124           ~ 190 2
2 SN 2007J SN* 02 18 51.70 +33 43 43.3     18.2     SNIbpec 39 1
3 SN 2005ek SN* 03 05 48.96 +36 46 10.6     17.5     SNIc: 76 1
4 SN 2010X SN* 04 48 27.90 +73 28 14.8           SNIc 85 1
5 SN 2002bj SN* 05 11 46.41 -15 08 10.8     14.8     SNIIn 86 1
6 SN 1939B SN* 12 42 02 +11 37.9   12.3       SNI 55 1
7 SN 2004cs SN* 17 50 14.38 +14 16 59.5   18.16 18.0     SNIa: 45 1

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