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首页> 外文期刊>The Astrophysical journal >THE GALACTIC DISTRIBUTION OF ALIPHATIC HYDROCARBONS IN THE DIFFUSE INTERSTELLAR MEDIUM
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THE GALACTIC DISTRIBUTION OF ALIPHATIC HYDROCARBONS IN THE DIFFUSE INTERSTELLAR MEDIUM

机译:弥散星际介质中脂肪烃的银河分布

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The infrared absorption feature near 2950 cm~(-1) (3.4 μm), characteristic of dust in the diffuse interstellar medium (ISM), is attributed to C—H stretching vibrations of aliphatic hydrocarbons. We show here that the strength of the band does not scale linearly with visual extinction everywhere, but instead increases more rapidly for objects near the center of the Galaxy, a behavior that parallels that of the Si—O stretching band due to silicate materials in the diffuse ISM. This implies that the grains responsible for the diffuse medium aliphatic C—H and silicate Si—O stretching bands are different from those responsible for much of the observed visual extinction. It also suggests that the distribution of the carbonaceous component of the diffuse ISM is not uniform throughout the Galaxy, but instead may increase in density toward the center of the Galaxy. The similar behavior of the C—H and Si—O stretching bands suggests that these two components may be coupled, perhaps in the form of silicate-core, organic-mantle grains. Several possible models of the distribution of this material are presented and it is demonstrated that the inner parts of the Galaxy has a carrier density that is 5 to 35 times higher than in the local ISM. Depending on the model used, the density of aliphatic material in the local ISM is found to be about 1 to 2 — CH_3 groups m~(-3) and about 2 to 5 —CH_2— groups m~(-3). These densities are consistent with the strengths of the 2955 and 2925 cm~(-1) (3.38 and 3.42 μm) subfeatures (due to — CH_3 and —CH_2— groups, respectively) within the overall 2950 cm~(-1) (3.4 μm) band being described by the relations A_v/τ_((2955 cm~(-1))) = 270 ± 40 and A_v/τ_((2925 cm~(-1))) = 250 ± 40 in the local diffuse ISM.
机译:2950 cm〜(-1)(3.4μm)附近的红外吸收特征是弥散星际介质(ISM)中的尘埃特征,归因于脂肪烃的CH拉伸振动。我们在这里表明,该带的强度并不是随处可见的消光而线性变化的,而是随着银河中心附近物体的增加而增加,这种行为与Si-O拉伸带的行为相似,这归因于硅中的硅酸盐材料。散布ISM。这意味着负责弥散介质脂肪族CH和硅酸盐Si-O拉伸带的晶粒与导致大部分观察到的视觉消光的晶粒不同。这也表明,弥散ISM中碳质成分的分布在整个银河系中并不均匀,而是可能朝银河系中心增加密度。 CHH和Si-O拉伸带的相似行为表明,这两个组分可能以硅酸盐核,有机幔颗粒的形式耦合。介绍了这种材料分布的几种可能模型,并证明了银河内部的载流子密度是当地ISM的5至35倍。根据所使用的模型,发现局部ISM中的脂肪族材料的密度为约1至2-CH_3基团m〜(-3)和约2至5 -CH 2-基团m〜(-3)。这些密度与整体2950 cm〜(-1)内的2955和2925 cm〜(-1)(分别为3.38和3.42μm)子特征(分别归因于-CH_3和-CH_2-)的强度一致。 μm)频带在局部扩散ISM中由关系A_v /τ_((2955 cm〜(-1)))= 270±40和A_v /τ_((2925 cm〜(-1)))= 250±40描述。

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