论文标题
对M型AGB星的ALF线排放的首次检测
First detection of AlF line emission towards M-type AGB stars
论文作者
论文摘要
氟(F)的核合成产生仍然是争论的问题。渐近巨型分支(AGB)恒星是F生产的主要候选者之一。但是,由于缺乏观察结果,它们对总F预算的贡献尚不完全了解。在本文中,我们报告了ALF线排放的检测,这是进化恒星流出中F的两个主要载体之一,朝着附近的五个富含氧气的AGB恒星,$ o $ o $ CETI,R LEO,IK TAU,R DOR,R DOR和W HYA。从空间解析的观测值中,我们估计了$ o $ CETI的半径$ \ sim11r _ {\ star} $和$ \ sim9r _ {\ star} $的ALF发射区域。根据人口图分析,我们报告了$ \ sim 5.8 \ times10^{15} $ cm $^{ - 2} $和$ \ sim 3 \ sim 3 \ times10^{15} $ cm $^{ - 2} $分别在这些地区内的ALF列密度。对于$ o $ $ ceti,我们使用了c $^{18} $ o($ v = 0 $,$ j = 3-2 $)观察值来估计发射区域的H $ _2 $列密度。我们发现$ f _ {\ rm alf/h_2} \ sim(2.5 \ pm1.7)\ times10^{ - 8} $的分数丰度。这给出了$ o $ CETI中F预算的下限,并且与太阳能F预算$ f _ {\ rm f/h_2} =(5 \ pm2)\ times10^{ - 8} $兼容。对于r leo,估计了分数丰度$ f _ {\ rm alf/h_2} =(1.2 \ pm0.5)\ times10^{ - 8} $。对于其他来源,我们无法根据可用数据精确确定发射区域。假设一个半径为$ \ sim 11r _ {\ star} $的发射区域,以及$ o $ $ ceti和r leo的旋转温度,我们粗略地将alf柱密度近似为$ \ sim(1.2-1.5)\ times10^{15} {15} $ cm $ cm $ cm $^{15} $ cm $^{ - 2} $ $ \ sim(2.5-3.0)\ times10^{14} $ cm $^{ - 2} $在r dor中,$ \ sim(0.6-1.0)\ times10^{16} $ cm $^{ - 2} $在ik tau中。这些结果导致$ f _ {\ rm alf/h_2} \ sim(0.1-4)\ times10^{ - 8} $在w hya,r dor和ik tau中的范围内。
The nucleosynthesis production of fluorine (F) is still a matter of debate. Asymptotic giant branch (AGB) stars are one of the main candidates for F production. However, their contribution to the total F budget is not fully known due to the lack of observations. In this paper, we report the detection of AlF line emission, one of the two main carriers of F in the gas-phase in the outflow of evolved stars, towards five nearby oxygen-rich AGB stars, $o$ Ceti, R Leo, IK Tau, R Dor, and W Hya. From spatially resolved observations, we estimated the AlF emitting region with a radius $\sim11R_{\star}$ for $o$ Ceti and $\sim9R_{\star}$ for R Leo. From population diagram analysis, we report the AlF column densities of $\sim 5.8\times10^{15}$ cm$^{-2}$ and $\sim 3\times10^{15}$ cm$^{-2}$ for $o$ Ceti and R Leo, respectively, within these regions. For $o$ Ceti, we used the C$^{18}$O ($v=0$, $J=3-2$) observations to estimate the H$_2$ column density of the emitting region. We found a fractional abundance of $f_{\rm AlF/H_2}\sim(2.5\pm1.7)\times10^{-8}$. This gives a lower limit on the F budget in $o$ Ceti and is compatible with the solar F budget $f_{\rm F/H_2}=(5\pm2)\times10^{-8}$. For R Leo, a fractional abundance $f_{\rm AlF/H_2}=(1.2\pm0.5)\times10^{-8}$ is estimated. For other sources, we cannot precisely determine the emitting region based on the available data. Assuming an emitting region with a radius of $\sim 11R_{\star}$ and the rotational temperatures derived for $o$ Ceti and R Leo, we crudely approximated the AlF column density to be $\sim(1.2-1.5)\times10^{15}$ cm$^{-2}$ in W Hya, $\sim(2.5-3.0)\times10^{14}$ cm$^{-2}$ in R Dor, and $\sim(0.6-1.0)\times10^{16}$ cm$^{-2}$ in IK Tau. These result in fractional abundances within a range of $f_{\rm AlF/H_2}\sim(0.1-4)\times10^{-8}$ in W Hya, R Dor, and IK Tau.