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arXiv 1801.03461astro-ph.GA
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在L1157-B1中寻找氰基多炔

A search for Cyanopolyynes in L1157-B1

E. Mendoza, B. Lefloch, C. Ceccarelli, C. Kahane, A. A. Jaber, L. Podio, M. Benedettini, C. Codella, S. Viti, I. Jimenez-Serra, J. Lepine, H. M. Boechat-Roberty, R. Bachiller

摘要:

本文介绍了利用IRAM 30米望远镜对太阳型恒星形成区进行化学观测的大型天体化学观测计划(ASAI)框架下,对激波区L1157-B1及其原恒星L1157-mm中的氰基多炔进行的系统搜索。在72和272 GHz之间的毫米窗口观测允许探测HC $_3$ N及其$^{13}$ C同位素,以及HC $_5$ N(首次在原恒星激波区)。在激波中,对谱线轮廓的分析表明,发射来自与L1157-B1和L1157-B2有关的流出空腔。分子丰度和激发条件从分析的谱线能量分布的假设下的局部热力学平衡或使用辐射转移代码中的大速度梯度近似。在L1157 mm附近,HC $_3$ N辐射来自冷包层($T_{rot}=10$ K)和原恒星周围较小范围的高激发区($T_{rot}$ = $31$ K)。我们没有发现任何证据表明$^{13}$ C或D分馏富集到L1157-B1。我们得到了冲击气体中HC $_3$ N/HC $_5$ N的相对丰度比为3.3。我们发现在L1157-mm的包络线和激波区域之间HC $_3$ N丰度增加了30倍。总之,这些结果与大部分HC $_3$ N是通过激波通道中的气相反应产生的情况一致。这种情况下,支持的参数冲击代码的预测与化学模型UCL_CHEM。

英文摘要:

We present here a systematic search for cyanopolyynes in the shock region L1157-B1 and its associated protostar L1157-mm in the framework of the Large Program "Astrochemical Surveys At IRAM" (ASAI), dedicated to chemical surveys of solar-type star forming regions with the IRAM 30m telescope. Observations of the millimeter windows between 72 and 272 GHz permitted the detection of HC$_3$N and its $^{13}$C isotopologues, and HC$_5$N (for the first time in a protostellar shock region). In the shock, analysis of the line profiles shows that the emission arises from the outflow cavities associated with L1157-B1 and L1157-B2. Molecular abundances and excitation conditions were obtained from analysis of the Spectral Line Energy Distributions under the assumption of Local Thermodynamical Equilibrium or using a radiative transfer code in the Large Velocity Gradient approximation. Towards L1157mm, the HC$_3$N emission arises from the cold envelope ($T_{rot}=10$ K) and a higher-excitation region ($T_{rot}$= $31$ K) of smaller extent around the protostar. We did not find any evidence of $^{13}$C or D fractionation enrichment towards L1157-B1. We obtain a relative abundance ratio HC$_3$N/HC$_5$N of 3.3 in the shocked gas. We find an increase by a factor of 30 of the HC$_3$N abundance between the envelope of L1157-mm and the shock region itself. Altogether, these results are consistent with a scenario in which the bulk of HC$_3$N was produced by means of gas phase reactions in the passage of the shock. This scenario is supported by the predictions of a parametric shock code coupled with the chemical model UCL_CHEM.

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