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NUCLEOSYNTHESIS IN TWO-DIMENSIONAL DELAYED DETONATION MODELS OF TYPE Ia SUPERNOVA EXPLOSIONS

K. MaedaInstitute for the Physics and Mathematics of the Universe (IPMU), University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba 277-8583, Japan; [email protected]F.K. RöpkeMax-Planck-Institut für Astrophysik, Karl-Schwarzschild-Straße 1, 85741 Garching, GermanyM. FinkMax-Planck-Institut für Astrophysik, Karl-Schwarzschild-Straße 1, 85741 Garching, GermanyW. HillebrandtMax-Planck-Institut für Astrophysik, Karl-Schwarzschild-Straße 1, 85741 Garching, GermanyC. TravaglioINAF-Osservatorio Astronomico di Torino, Strada dell’Osservatorio 20, I-10025 Pino Torinese, Torino, ItalyF.-K. ThielemannDepartment Physik, Universität Basel, CH-4056 Basel, Switzerland
2010en
ABI

Аннотация

The nucleosynthetic characteristics of various explosion mechanisms of Type Ia supernovae (SNe Ia) is explored based on three two-dimensional explosion simulations representing extreme cases: a pure turbulent deflagration, a delayed detonation following an approximately spherical ignition of the initial deflagration, and a delayed detonation arising from a highly asymmetric deflagration ignition. Apart from this initial condition, the deflagration stage is treated in a parameter-free approach. The detonation is initiated when the turbulent burning enters the distributed burning regime. This occurs at densities around $10^{7}$ g cm$^{-3}$ -- relatively low as compared to existing nucleosynthesis studies for one-dimensional spherically symmetric models. The burning in these multidimensional models is different from that in one-dimensional simulations as the detonation wave propagates both into unburned material in the high density region near the center of a white dwarf and into the low density region near the surface. Thus, the resulting yield is a mixture of different explosive burning products, from carbon-burning products at low densities to complete silicon-burning products at the highest densities, as well as electron-capture products synthesized at the deflagration stage. In contrast to the deflagration model, the delayed detonations produce a characteristic layered structure and the yields largely satisfy constraints from Galactic chemical evolution. In the asymmetric delayed detonation model, the region filled with electron capture species (e.g., $^{58}$Ni, $^{54}$Fe) is within a shell, showing a large off-set, above the bulk of $^{56}$Ni distribution, while species produced by the detonation are distributed more spherically (abridged).

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