2011/03/31 by David A. Chamulak, Casey A. Meakin, Ivo R. Seitenzahl +1
Physics and Astronomy · #Adiabatic process #Asymmetry #Deflagration #Detonation #Ejecta #Gamma-ray bursts and supernovae #Mass distribution #Neutrino Physics Research #Pulsars and Gravitational Waves Research #Supernova #White dwarf #astro-ph.SR
paper · pdf · doi:10.1088/0004-637x/744/1/27
7 pages, 7 figures, accepted for publication in the Astrophysical Journal
arxiv created 2011/09/16 · openalex publication_date 2011/12/09 · arxiv updated 2015/05/27 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Most of the leading explosion scenarios for Type Ia supernovae involve the nuclear incineration of a white dwarf star through a detonation wave. Several scenarios have been proposed as to how this detonation may actually occur, but the exact mechanism and environment in which it takes place remain unknown. We explore the effects of an off-center initiated detonation on the spatial distribution of the nucleosynthetic yield products in a toy model—a pre-expanded near Chandrasekhar-mass white dwarf. We find that a single-point near edge-lit detonation results in asymmetries in the density and thermal profiles, notably the expansion timescale, throughout the supernova ejecta. We demonstrate that this asymmetry of the thermodynamic trajectories should be common to off-center detonations where a small amount of the star is burned prior to detonation. The sensitivity of the yields on the expansion timescale results in an asymmetric distribution of the elements synthesized as reaction products. We tabulate the shift in the center of mass of the various elements produced in our model supernova and find an odd–even pattern for elements past silicon. Our calculations show that off-center single-point detonations in carbon–oxygen white dwarfs are marked by significant composition asymmetries in their remnants which bear potentially observable signatures in both velocity and coordinate space, including an elemental nickel mass fraction that varies by a factor of 2–3 from one side of the remnant to the other.