GG Tau A 盘中的化学:来自 H2D+、N2H+ 和 DCO+ 高角分辨率 ALMA 观测的制约因素

Parashmoni Kashyap, Liton Majumdar, Anne Dutrey, Stéphane Guilloteau, Karen Willacy, Edwige Chapillon, Richard Teague, Dmitry Semenov, Thomas Henning, Neal Turner, Raghvendra Sahai, Ágnes Kóspál, Audrey Coutens, V. Piétu, Pierre Gratier, Maxime Ruaud, N. T. Phuong, E. Di Folco, Chin-Fei Lee and Y.-W. Tang
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引用次数: 0

摘要

分辨分子线观测对于深入了解原行星盘的物理和化学结构至关重要,尤其是在行星形成并获得其化学成分的低温致密区域。然而,对这些区域进行追踪具有挑战性,因为大多数分子冻结在颗粒表面,在气相中无法观测。我们利用阿塔卡马大型毫米波/亚毫米波阵列(ALMA)波段 7 的观测数据研究了金牛座三恒星盘 GG Tau A 中的冷分子化学反应,该盘中有一个大质量气体和尘埃环以及一个外盘。我们展示了 N2H+ 和 DCO+ 发射的高角分辨率地图,并报告了 H2D+、13CS 和 SO2 的上限。N2H+ 的径向强度分布图显示了环外缘附近的大部分发射,而 DCO+ 则显示了双峰值,一个在环内缘附近,另一个在外盘。通过对低层跃迁的补充观测,我们确定了分子表面密度和旋转温度。我们比较了不同宇宙射线电离率(CRI)、碳氧比(C/O)和恒星紫外线通量下的推导量和模型预测量。影响 N2H+、DCO+ 和 H2D+ 丰度的冷分子化学对 CRI 率最为敏感,而恒星紫外线通量和碳氧比对这三种离子的影响最小。我们的最佳模型需要 10-18 s-1 的低有源离子强度。然而,它无法与 N2H+ 和 DCO+ 的低温(12-16 K)相匹配,这比 CO 的凝固温度要低得多。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Chemistry in the GG Tau A Disk: Constraints from H2D+, N2H+, and DCO+ High Angular Resolution ALMA Observations
Resolved molecular line observations are essential for gaining insight into the physical and chemical structure of protoplanetary disks, particularly in cold, dense regions where planets form and acquire their chemical compositions. However, tracing these regions is challenging because most molecules freeze onto grain surfaces and are not observable in the gas phase. We investigated cold molecular chemistry in the triple stellar T Tauri disk GG Tau A, which harbours a massive gas and dust ring and an outer disk, using Atacama Large Millimeter/submillimeter Array (ALMA) Band 7 observations. We present high angular resolution maps of N2H+ and DCO+ emission, with upper limits reported for H2D+, 13CS, and SO2. The radial intensity profile of N2H+ shows most emission near the ring’s outer edge, while DCO+ exhibits a double peak, one near the ring’s inner edge and the other in the outer disk. With complementary observations of lower-lying transitions, we constrained the molecular surface densities and rotation temperatures. We compared the derived quantities with model predictions across different cosmic-ray ionization (CRI) rates, carbon-to-oxygen (C/O) ratios, and stellar UV fluxes. Cold molecular chemistry, affecting the N2H+, DCO+, and H2D+ abundances, is most sensitive to the CRI rate, while the stellar UV fluxes and C/O ratios have minimal impact on these three ions. Our best model requires a low CRI rate of 10−18 s−1. However, it fails to match the low temperatures derived from N2H+ and DCO+, 12–16 K, which are much lower than the CO freezing temperature.
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