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The deuterium fractionation of water on solar-system scales in deeply-embedded low-mass protostars

机译:深埋低质量原恒星中太阳系尺度上水的氘分馏

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Context. The chemical evolution of water through the star formation process directly affects the initial conditions of planet formation. The water deuterium fractionation (HDO/H2O abundance ratio) has traditionally been used to infer the amount of water brought to Earth by comets. Measuring this ratio in deeply-embedded low-mass protostars makes it possible to probe the critical stage when water is transported from clouds to disks in which icy bodies are formed. Aims. We aim to determine the HDO/H2O abundance ratio in the warm gas in the inner 150 AU for three deeply-embedded low-mass protostars NGC 1333-IRAS 2A, IRAS 4A-NW, and IRAS 4B through high-resolution interferometric observations of isotopologues of water. Methods. We present sub-arcsecond resolution observations of the 31,2?22,1 transition of HDO at 225.89672 GHz in combination with previous observations of the 31,3?22,0 transition of H218O at 203.40752 GHz from the Plateau de Bure Interferometer toward three low-mass protostars. The observations have similar angular resolution (0.?7–1.?3), probing scales R???150 AU. In addition, observations of the 21,1?21,2 transition of HDO at 241.561 GHz toward IRAS 2A are presented to constrain the excitation temperature. A direct and model independent HDO/H2O abundance ratio is determined for each source and compared with HDO/H2O ratios derived from spherically symmetric full radiative transfer models for two sources. Results. From the two HDO lines observed toward IRAS 2A, the excitation temperature is found to be Tex?=?124?±?60 K. Assuming a similar excitation temperature for H218O and all sources, the HDO/H2O ratio is 7.4?±?2.1?×?10-4 for IRAS 2A, 19.1?±?5.4?×?10-4 for IRAS 4A-NW, and 5.9?±?1.7?×?10-4 for IRAS 4B. The abundance ratios show only a weak dependence on the adopted excitation temperature. The abundances derived from the radiative transfer models agree with the direct determination of the HDO/H2O abundance ratio for IRAS 16293-2422 within a factor of 2–3, and for IRAS 2A within a factor of 4; the difference is mainly due to optical depth effects in the HDO line. Conclusions. Our HDO/H2O ratios for the inner regions (where T?>?100 K) of four young protostars are only a factor of 2 higher than those found for pristine, solar system comets. These small differences suggest that little processing of water occurs between the deeply embedded stage and the formation of planetesimals and comets.
机译:上下文。水通过恒星形成过程的化学演化直接影响行星形成的初始条件。传统上已使用水氘分馏(HDO / H2O丰度比)来推断彗星带入地球的水量。在深层埋藏的低质量原恒星中测量该比率可以探测水从云层传输到形成冰体的磁盘的关键阶段。目的我们旨在通过高分辨率同位素计量干涉观察法,确定三个深埋的低质量原恒星NGC 1333-IRAS 2A,IRAS 4A-NW和IRAS 4B在150 AU内部150 AU内暖气体中HDO / H2O的丰度比。水。方法。我们提出了225.89672 GHz下HDO的31,2?22,1跃迁的亚弧分辨率观测结果,以及先前从高原干扰仪向203向40,3752 GHz处H218O的31,3?22,0跃迁的观测结果,低质量的原星。观测值具有相似的角分辨率(0.?7-1?.3),探测比例尺为R ??? 150 AU。另外,提出了对HDO在241.561 GHz处向IRAS 2A的21,1→21,2跃迁的观察,以限制激发温度。确定每个源的直接且独立于模型的HDO / H2O丰度比,并将其与从两个源的球对称全辐射传输模型得出的HDO / H2O比值进行比较。结果。从朝向IRAS 2A观察到的两条HDO线,发现激发温度为Texα=?124?±?60K。假设H218O和所有源的激发温度相似,则HDO / H2O比为7.4?±?2.1。 IRAS 2A为××10-4,IRAS 4A-NW为19.1±α5.4××10-4,IRAS 4B为5.9±±1.7××10-4。丰度比显示对所采用的激发温度的依赖性很小。从辐射传输模型得出的丰度与直接确定IRAS 16293-2422的HDO / H2O丰度比在2到3的范围内,对于IRAS 2A的HDO / H2O丰度比的直接确定在4的范围内一致。差异主要是由于HDO线路中的光学深度效应。结论。我们的四个年轻原恒星内部区域的HDO / H2O比(T> 100K时)仅比原始的太阳系彗星高2倍。这些微小差异表明,在深埋阶段与小行星和彗星的形成之间几乎没有水的处理。

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