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ORTHO-TO-PARA RATIO STUDIES OF SHOCKED H2 GAS IN THE TWO SUPERNOVA REMNANTS IC?443 AND HB?21

机译:两种超新星残渣IC?443和HB?21中H2气体的正交比对研究

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We present near-infrared (2.5-5.0 μm) spectral studies of shocked H2 gas in two supernova remnants, IC?443 and HB?21, which are well known for their interactions with nearby molecular clouds. The observations were performed with the Infrared Camera aboard the AKARI satellite. At the energy range 7000?K? ? 20,000?K, the shocked H2 gas in IC?443 shows an ortho-to-para ratio (OPR) of 2.4+0.3 – 0.2, which is significantly lower than the equilibrium value 3, suggesting the existence of non-equilibrium OPR. The shocked gas in HB?21 also indicates a potential non-equilibrium OPR in the range of 1.8-2.0. The level populations are well described by the power-law thermal admixture model with a single OPR, where the temperature integration range is 1000-4000?K. We conclude that the obtained non-equilibrium OPR probably originates from the reformed H2 gas of dissociative J-shocks, considering several factors such as the shock combination requirement, the line ratios, and the possibility that H2 gas can form on grains with a non-equilibrium OPR. We also investigate C-shocks and partially dissociative J-shocks as the origin of the non-equilibrium OPR. However, we find that they are incompatible with the observed ionic emission lines for which dissociative J-shocks are required to explain. The difference in the collision energy of H atoms on grain surfaces would give rise to the observed difference between the OPRs of IC?443 and HB?21, if dissociative J-shocks are responsible for the H2 emission. Our study suggests that dissociative J-shocks can produce shocked H2 gas with a non-equilibrium OPR.
机译:我们目前对两个超新星残余物IC?443和HB?21中的H2气体的冲击波进行近红外(2.5-5.0μm)光谱研究,它们以与附近分子云的相互作用而闻名。观察是用AKARI卫星上的红外摄像机进行的。在能量范围7000?K? ?在20,000?K下,IC?443中的H2气体表现出的正对对数比(OPR)为2.4 + 0.3 – 0.2,显着低于平衡值3,表明存在非平衡OPR。 HB?21中的冲击气体还表明潜在的非平衡OPR在1.8-2.0范围内。能级分布可以通过具有单个OPR的幂律热混合模型很好地描述,其中温度积分范围为1000-4000?K。我们得出的结论是,考虑到多种因素,例如冲击组合要求,线宽比以及在具有非结晶性的晶粒上形成氢气的可能性,获得的非平衡原核磁共振可能源自离解J型冲击的重整氢气。平衡OPR。我们还研究了C震荡和部分解离J震荡作为非平衡OPR的起源。但是,我们发现它们与观察到的离子发射谱线不兼容,对于这些离子发射谱线,需要用解离性J型冲击来解释。如果解离的J型激波负责H2的发射,则H原子在晶粒表面上的碰撞能量的差异将导致IC?443和HB?21的OPR之间观察到差异。我们的研究表明,解离的J型冲击波可以通过非平衡OPR产生冲击氢气。

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