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Nucleosynthesis in Chandrasekhar Mass Models for Type Ia Supernovae and Constraints on Progenitor Systems and Burning-Front Propagation

机译:Ia型超新星和河流的Chandrasekhar质量模型的核合成   祖先系统和燃烧前沿传播的制约因素

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摘要

We calculate explosive nucleosynthesis in Chandrasekhar mass models for TypeIa Supernovae(SNe Ia) to obtain new constraints on the rate of matter accretiononto the progenitor white dwarf and on the ignition density of central carbondeflagration. The calculated abundance of the Fe-group neutron-rich nuclei ishighly sensitive to the electron captures taking place in the central layers.The yields obtained from a slow central deflagration, and from a fastdeflagration or delayed detonation in the outer layers, are combined and put tocomparison with solar isotopic abundances. We found that (1) to avoid too largeratios of $^{54}$Cr/$^{56}$Fe and $^{50}$Ti/$^{56}$Fe, the ignition densityshould be as low as \ltsim 2 \e9 \gmc, and that (2) to avoid the overproductionof $^{58}$Ni and $^{54}$Fe, either the flame speed should not exceed a few % ofthe sound speed in the central low $Y_e$ layers, or the progenitor star has tobe metal-poor compared with solar. Such low central densities can be realizedby a rapid accretion as fast as $\dot M$ \gtsim 1 $\times$ 10$^{-7}$M$_\odot$yr$^{-1}$. In order to reproduce the solar abundance of $^{48}$Ca, one alsoneeds progenitor systems that undergo ignition at higher densities. We alsofound that the total amount of $^{56}$Ni, the Si-Ca/Fe ratio, and the abundanceof elements like Mn and Cr (incomplete Si-burning ashes), depend on the densityof the deflagration-detonation transition in delayed detonations. Ournucleosynthesis results favor transition densities slightly below 2.2$\times10^7$ g cm$^{-3}$.
机译:我们在Chandrasekhar质量模型中计算了TypeIa超新星(SNe Ia)的爆炸性核合成,从而获得了对祖先白矮星物质吸收速率和中心碳爆燃点火密度的新约束。计算得出的富铁中子富核的丰度对在中心层发生的电子捕获高度敏感,将慢速中心爆燃,外层快速爆燃或延迟爆震获得的产率合并并放入与太阳同位素丰度进行比较我们发现(1)为避免$ ^ {54} $ Cr / $ ^ {56} $ Fe和$ ^ {50} $ Ti / $ ^ {56} $ Fe的比例过大,点火密度应低至\ ltsim 2 \ e9 \ gmc,以及(2)为避免$ ^ {58} $ Ni和$ ^ {54} $ Fe的过量生产,火焰速度不应超过中央低处声速的百分之几$ Y_e $层,否则与太阳相比,祖先的恒星必须是金属贫乏的。如此低的中心密度可以通过快速积聚来实现,就像$ \ dot M $ \ gtsim 1 $ \ times $ 10 $ ^ {-7} $ M $ _ \ odot $ yr $ ^ {-1} $。为了再现$ ^ {48} $ Ca的太阳丰度,还需要一种以更高密度点火的祖先系统。我们还发现$ ^ {56} $ Ni的总量,Si-Ca / Fe比以及Mn和Cr之类元素的丰度(不完全的Si燃烧灰烬)取决于延迟时的爆燃-爆轰转变的密度。爆炸。我们的核合成结果有利于过渡密度略低于2.2 $ \ times10 ^ 7 $ g cm $ ^ {-3} $。

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