Ia型超新星Si i λ6355速度分布及其对不对称爆炸的启示

Keto D. Zhang, Wei Zheng, T. de Jaeger, B. Stahl, T. Brink, Xuhui Han, D. Kasen, K. Shen, Kevin Tang, A. Filippenko
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引用次数: 4

摘要

在研究Ia型超新星(SNe Ia)的结构和性质时,喷射速度是一个非常重要的参数。它也是提高超新星Ia在宇宙距离测定中的效用的候选关键参数。本文研究了kaepora数据库311 Ia震源的速度分布。速度是由测量(或外推)峰值亮度时间的光谱中的Si II $\lambda$ 6355吸收线导出的。我们统计表明,观测到的速度具有双峰高斯分布,由两组Ia型SNe组成:第一组具有较低但较窄的散点($\mu_1 = 11000 \text{km s}^{-1}$, $\sigma_1 = 700 \text{km s}^{-1}$),第二组具有较高但较宽的散点($\mu_2 = 12300 \text{km s}^{-1}$, $\sigma_2 = 1800 \text{km s}^{-1}$)。第一组和第二组的人口比例是201:110%:35%). There is substantial degeneracy between the two groups, but for SNe Ia with velocity $v > 12000 \text{km s}^{-1}$, the distribution is dominated by Group II. The true origin of the two components is unknown, though there could be that naturally there exist two intrinsic velocity distributions as observed. However, we try to use asymmetric geometric models through statistical simulations to reproduce the observed distribution assuming all SNe Ia share the same intrinsic distribution. In the two cases we consider, 35\% of SNe Ia are considered to be asymmetric in Case 1, and all SNe Ia are asymmetric in Case 2. Simulations for both cases can reproduce the observed velocity distribution but require a significantly large portion ($>35\%$) of SNe Ia to be asymmetric. In addition, the Case 1 result is consistent with recent polarization observations that SNe Ia with higher Si II $\lambda$6355 velocity tend to be more polarized.
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Distribution of Si ii λ6355 velocities of Type Ia supernovae and implications for asymmetric explosions
The ejecta velocity is a very important parameter in studying the structure and properties of Type Ia supernovae (SNe Ia). It is also a candidate key parameter in improving the utility of SNe Ia for cosmological distance determinations. Here we study the velocity distribution of a sample of 311 SNe Ia from the kaepora database. The velocities are derived from the Si II $\lambda$6355 absorption line in optical spectra measured at (or extrapolated to) the time of peak brightness. We statistically show that the observed velocity has a bimodal Gaussian distribution consisting of two groups of SNe Ia: Group I with a lower but narrower scatter ($\mu_1 = 11000 \text{km s}^{-1}$, $\sigma_1 = 700 \text{km s}^{-1}$), and Group II with a higher but broader scatter ($\mu_2 = 12300 \text{km s}^{-1}$, $\sigma_2 = 1800 \text{km s}^{-1}$). The population ratio of Group I to Group II is 201:110 (65%:35%). There is substantial degeneracy between the two groups, but for SNe Ia with velocity $v > 12000 \text{km s}^{-1}$, the distribution is dominated by Group II. The true origin of the two components is unknown, though there could be that naturally there exist two intrinsic velocity distributions as observed. However, we try to use asymmetric geometric models through statistical simulations to reproduce the observed distribution assuming all SNe Ia share the same intrinsic distribution. In the two cases we consider, 35\% of SNe Ia are considered to be asymmetric in Case 1, and all SNe Ia are asymmetric in Case 2. Simulations for both cases can reproduce the observed velocity distribution but require a significantly large portion ($>35\%$) of SNe Ia to be asymmetric. In addition, the Case 1 result is consistent with recent polarization observations that SNe Ia with higher Si II $\lambda$6355 velocity tend to be more polarized.
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