首页> 外文OA文献 >The water abundance behind interstellar shocks: results from $Herschel$/PACS and $Spitzer$/IRS observations of H$_2$O, CO, and H$_2$
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The water abundance behind interstellar shocks: results from $Herschel$/PACS and $Spitzer$/IRS observations of H$_2$O, CO, and H$_2$

机译:星际冲击背后的水丰度:来自   $ Herschel $ / paCs和$ spitzer $ / IRs对H $ _ $ O $,CO和H $ _ $ 2的观察

摘要

We have investigated the water abundance in shock-heated molecular gas,making use of $Herschel$ measurements of far-infrared CO and H$_2$O lineemissions in combination with $Spitzer$ measurements of mid-IR H$_2$ rotationalemissions. We present far-infrared line spectra obtained with $Herschel$'s PACSinstrument in range spectroscopy mode towards two positions in the protostellaroutflow NGC 2071 and one position each in the supernova remnants W28 and 3C391.These spectra provide unequivocal detections, at one or more positions, of 12rotational lines of water, 14 rotational lines of CO, 8 rotational lines of OH(4 lambda doublets), and 7 fine-structure transitions of atoms or atomic ions.We first used a simultaneous fit to the CO line fluxes, along with H$_2$rotational line fluxes measured previously by $Spitzer$, to constrain thetemperature and density distribution within the emitting gas; and we theninvestigated the water abundances implied by the observed H$_2$O line fluxes.The water line fluxes are in acceptable agreement with standard theoreticalmodels for nondissociative shocks that predict the complete vaporization ofgrain mantles in shocks of velocity $v \sim 25$ km/s, behind which thecharacteristic gas temperature is $\sim 1300$ K and the H$_2$O/CO ratio is 1.2
机译:我们通过对远红外CO和H $ _2 $ O线发射的$ Herschel $测量以及对IR中线H $ _2 $旋转发射的$ Spitzer $测量相结合,研究了冲击加热分子气体中的水丰度。我们展示了由$ Herschel $的PACS仪器在距离光谱模式下获得的远红外谱线,指向原恒星流出NGC 2071中的两个位置,以及超新星遗迹W28和3C391中的每个位置,这些光谱提供了一个或多个位置的明确检测。 ,12条水的旋转线,14条CO的旋转线,8条OH(4 lambda doublets)的旋转线以及7个原子或原子离子的精细结构转变。我们首先对CO线通量同时拟合H $ _2 $旋转线通量以前由Spitzer $测量,以限制发射气体中的温度和密度分布;然后我们研究了观察到的H $ _2 $ O线通量所隐含的水丰度。水线通量与非解离性冲击的标准理论模型相一致,该模型预测了速度$ v \ sim 25 $ km的冲击中颗粒幔的完全蒸发/ s,其后的特征气体温度为$ \ sim 1300 $ K,H $ _2 $ O / CO比为1.2

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