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arXiv 2307.04487astro-ph.GA
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星际云中分子阴离子的丰度与激发

The abundance and excitation of molecular anions in interstellar clouds

M. Agundez, N. Marcelino, B. Tercero, I. Jimenez-Serra, J. Cernicharo

AI总结:

本文利用 Yebes 40m 和 IRAM 30m 望远镜观测星际冷致密云中的分子阴离子,首次探测到多种阴离子并报告新谱线,通过激发计算与丰度建模,发现阴离子与中性分子比值随分子尺寸增大而增加,支持辐射电子附着形成机制。

摘要:

我们报告了使用 Yebes 40m 和 IRAM 30m 望远镜对冷致密云 TMC-1 CP、Lupus-1A、L1527、L483、L1495B 和 L1544 进行的分子阴离子新观测结果。我们首次在 Lupus-1A 中探测到了 C3N- 和 C5N-,并在 L483 中探测到了 C4H- 和 C6H-。此外,我们报告了在六个目标源中观测到的 C6H- 新谱线,在 TMC-1 CP、Lupus-1A 和 L1527 中观测到的 C4H- 新谱线,以及在 TMC-1 CP 中观测到的 C8H- 和 C3N- 谱线。激发计算表明,射电望远镜可探测到的阴离子谱线从亚热激发到热化状态不等,随着阴离子尺寸的增加而变化,其偏离热化的程度取决于 H2 体积密度和谱线频率。我们注意到,目前可用的自由基 C6H 碰撞速率系数无法解释多项观测事实,这建议需要重新审视该物种的碰撞数据。本文提出的观测结果,连同文献中的观测数据,被用于模拟星际阴离子的激发并约束其丰度。总体而言,当有文献值可供对比时,本文推导出的阴离子与中性分子之比在 50%(最多两倍因子)的误差范围内与文献值一致,但 C4H-/C4H 比值除外,该比值由于对 C4H 偶极矩的修订而显示出较大差异。从推导出的一组阴离子与中性分子丰度比中可以得出两个结论。首先,C6H-/C6H 比值呈现出一种初步趋势,即该比值随 H2 密度的增加而增加,这与理论基础预期相符。其次,不可否认的是,分子尺寸越大,阴离子与中性分子的比值就越高,这支持了基于辐射电子附着机制的形成理论。尽管如此,计算得出的中等尺寸物种 C4H 和 C3N 的电子附着速率系数可能分别偏高和偏低了一到两个数量级。

英文摘要:

We report new observations of molecular anions with the Yebes 40m and IRAM 30m telescopes toward the cold dense clouds TMC-1 CP, Lupus-1A, L1527, L483, L1495B, and L1544. We detected for the first time C3N- and C5N- in Lupus-1A and C4H- and C6H- in L483. In addition, we report new lines of C6H- toward the six targeted sources, of C4H- toward TMC-1 CP, Lupus-1A, and L1527, and of C8H- and C3N- in TMC-1 CP. Excitation calculations indicate that the lines of anions accessible to radiotelescopes run from subthermally excited to thermalized as the size of the anion increases, with the degree of departure from thermalization depending on the H2 volume density and the line frequency. We noticed that the collision rate coefficients available for the radical C6H cannot explain various observational facts, which advises for a revisitation of the collision data for this species. The observations presented here, together with observational data from the literature, are used to model the excitation of interstellar anions and to constrain their abundances. In general, the anion-to-neutral ratios derived here agree within 50 % (a factor of two at most) with literature values, when available, except for the C4H-/C4H ratio, which shows higher differences due to a revision of the dipole moment of C4H. From the set of anion-to-neutral abundance ratios derived two conclusions can be drawn. First, the C6H-/C6H ratio shows a tentative trend in which it increases with increasing H2 density, as expected from theoretical grounds. And second, it is incontestable that the higher the molecular size the higher the anion-to-neutral ratio, which supports a formation mechanism based on radiative electron attachment. Nonetheless, calculated rate coefficients for electron attachment to the medium size species C4H and C3N are probably too high and too low, respectively, by more than one order of magnitude.

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