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The Laminar Flame Speedup by 22Ne Enrichment in White Dwarf Supernovae

David A. Chamulak et al 2007 ApJ 655 L93-L96   doi: 10.1086/511856  Help

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David A. Chamulak1, Edward F. Brown1,3 and Francis X. Timmes2
1 Department of Physics and Astronomy and the Joint Institute for Nuclear Astrophysics, Michigan State University, East Lansing, MI
2 Thermonuclear Applications, Los Alamos National Laboratory, Los Alamos, NM
3 National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, MI
E-mail: chamulak@pa.msu.edu, ebrown@pa.msu.edu and timmes@lanl.gov

ABSTRACT. Carbon-oxygen white dwarfs contain 22Ne formed from α-captures onto 14N during core He burning in the progenitor star. In a white dwarf (Type Ia) supernova, the 22Ne abundance determines, in part, the neutron-to-proton ratio and hence the abundance of radioactive 56Ni that powers the light curve. The 22Ne abundance also changes the burning rate and hence the laminar flame speed. We tabulate the flame speedup for different initial 12C and 22Ne abundances and for a range of densities. This increase in the laminar flame speed—about 30% for a 22Ne mass fraction of 6%—affects the deflagration just after ignition near the center of the white dwarf, where the laminar speed of the flame dominates over the buoyant rise, and in regions of lower density, ~107 g cm-3, where a transition to distributed burning is conjectured to occur. The increase in flame speed will decrease the density of any transition to distributed burning.

Subject headings: galaxies: evolution; nuclear reactions, nucleosynthesis, abundances; supernovae: general; white dwarfs

Print publication: Issue 2 (2007 February 1)
Received 2006 October 31, accepted for publication 2006 December 15
Published 2007 January 16

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