Dynamics of a Spherical Accretion Shock with Neutrino Heating and Alpha-Particle Recombination
Rodrigo Fernández, Christopher Thompson
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Published in ApJ. This version includes some proof corrections. Minor changes relative to submitted version (rephrasing of some statements, and updated figures 5, 6a, 9, 10, 12, 13, 14, 17). Version with high resolution figures at http://sns.ias.edu/~rafernan/alpha_movies.html
We investigate the effects of neutrino heating and alpha-particle recombination on the hydrodynamics of core-collapse supernovae. Our focus is on the non-linear dynamics of the shock wave that forms in the collapse, and the assembly of positive energy material below it. To this end, we perform time-dependent hydrodynamic simulations with FLASH2.5 in spherical and axial symmetry. These generalize our previous calculations by allowing for bulk neutrino heating and for nuclear statistical equilibrium between n, p and alpha. The heating rate is freely tunable, as is the starting radius of the shock relative to the recombination radius of alpha-particles. An explosion in spherical symmetry involves the excitation of an overstable mode, which may be viewed as the L=0 version of the `Standing Accretion Shock Instability'. In 2D simulations, non-spherical deformations of the shock are driven by plumes of material with positive Bernoulli parameter, which are concentrated well outside the zone of strong neutrino heating. The non-spherical modes of the shock reach a large amplitude only when the heating rate is also high enough to excite convection below the shock. The critical heating rate that causes an explosion depends sensitively on the initial position of the shock relative to the recombination radius. Weaker heating is required to drive an explosion in 2D than in 1D, but the difference also depends on the size of the shock. Forcing the infalling heavy nuclei to break up into n and p below the shock only causes a slight increase in the critical heating rate, except when the shock starts out at a large radius. This shows that heating by neutrinos (or some other mechanism) must play a significant role in pushing the shock far enough out that recombination heating takes over.
Electron-Ion Recombination Rate Coefficients and Photoionization Cross Sections for Astrophysically Abundant Elements. IX. Ni XXVI and Ni XXVII for UV and X-ray modeling
The Spin-Kinetic Temperature Coupling and the Heating Rate due to Lyman Alpha Scattering before Reionization: Predictions for 21cm Emission and Absorption
The evolution of a pre-heated Intergalactic Medium
我们分析了星系际介质(IGM)的演变,通过一套扩展的大盒子大小的流体动力学模拟,其中包括预热。我们着重讨论z~2 Lyman-alpha森林的性质以及z=0时星系团和星系群的布居。我们调查中的莱曼α通量和熵的星系群的温度关系的空洞的分布,比较模拟结果,从高分辨率的类星体光谱和X射线观测的最新数据。预热是通过一个简单的唯象公式来实现的,其中在z=4时,所有气体粒子的熵,其过密度超过阈值delta_h,增加到最小值K_fl。而在星系群中心区域观察到的熵水平需要相当强的预热,K_fl>100 keV cm ^2,莱曼-α森林的空隙统计学要求这种预热应该只发生在相对高密度的区域,以便不破坏产生森林的冷细丝。我们的结论是,任何注入的非引力能量的扩散重子应避免低密度区在高红移和/或发生在相对较低的红移。
Electron-Ion Recombination Rate Coefficients and Photoionization Cross Sections for Astrophysically Abundant Elements IV. Relativistic calculations for C IV and C V for UV and X-ray modeling
利用相对论Breit-Pauli R矩阵方法计算了类氦离子和类锂离子光电离和复合的第一套完整的统一截面和速率系数。我们提出了总的,统一的(e +离子)复合速率系数(e + C VI -> C V)和(e + C V \longrightarrow C IV),包括精细结构。特定级别的重组率系数的n = 10的水平也首次获得,这些有很大的不同,从目前可用的近似速率。指出了复合级联系数在类氦离子K α发射的X射线谱模型中的应用。总重组率的总体不确定性不应超过10- 20%。在日冕近似下,用新的速率重新计算了碳的电离分数。目前(电子+离子)的复合速率系数进行比较,与几组可用的数据,包括以前的LS耦合结果,和“实验得出的”速率系数。相对论精细结构的作用,共振,辐射阻尼,和干涉效应的分辨率进行了讨论。复合率的两个一般特征被注意到:(i)非共振(辐射复合)峰为E,T -> 0,和(ii)高T共振(双电子复合)峰。
CII* Absorption in Damped Lyman Alpha Systems: (I) Star Formation Rates in a Two-Phase Medium
我们描述了一种技术,第一次直接测量阻尼莱曼α系统(DLAs)中的恒星形成率(SFR)。我们假设大质量恒星形成于DLAs中,它们发出的FUV辐射通过颗粒光电机制加热气体。我们从由CII* 1335.7吸收强度测量的冷却速率推断出加热速率。由于加热速率与尘气比和单位面积的SFR成正比,因此我们推导出DLAs的单位面积SFR,其中这两个量都已测量。我们考虑模型中的灰尘包括碳质或硅酸盐颗粒。提出了冷中性介质(CNM)和暖中性介质(WNM)处于压力平衡的两相模型。在CNM模型中,视线穿过CNM和WNM,而在WNM模型中,视线仅穿过WNM。由于谷物的光电加热效率在CNM中至少比在WNM中高10倍,因此在CNM模型中,CII* 吸收主要发生在CNM中。但在WNM模型中,所有的CII* 吸收都发生在WNM中。我们使用CII* 的吸收线,以获得每单位面积的SFR的样品中的30 DLAs的灰尘,气体的比例已被推断从元素耗尽模式。我们表明,由此产生的每单位面积的SFR对应于平均超过恒星形成量的星系托管的DLA,而不是本地恒星形成沿视线。我们发现单位面积的平均SFR,对于CNM模型等于10 $^{-2.2}$ M $_{\odot}$ yr $^{-1}$ kpc $^{-2}$,对于WNM模型等于10 $^{-1.3}$ M $_{\odot}$ yr $^{-1}$ kpc $^{-2}$。CNM溶液…