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LARGE SILICON ABUNDANCE IN PHOTODISSOCIATION REGIONS

机译:光解区的大硅丰度

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We have made one-dimensional raster scan observations of the ρ Oph and σ Sco star-forming regions with two spectrometers (SWS and LWS) on board the ISO. In the ρ Oph region, [Si Ⅱ] 35 μm, [O Ⅰ] 63 μm, 146 μm, [C Ⅱ] 15 8 μm, and the H_2 pure rotational transition lines S(0) to S(3) are detected, and the photodissociation region (PDR) properties are derived as the radiation field scaled by the solar neighborhood value G_0 ~ 30-500, the gas density n ~ 250-2500 cm~(-3), and the surface temperature T ~ 100-400 K. The ratio of [Si Ⅱ] 35 μm to [O Ⅰ] 146 μm indicates that silicon of 10%-20% of the solar abundance must be in the gaseous form in the PDR, suggesting that efficient dust destruction is ongoing even in the PDR and that a fraction of the silicon atoms may be contained in volatile forms in dust grains. The [O Ⅰ] 63 μm and [C Ⅱ] 158 μm emissions are too weak relative to [O Ⅰ] 146 μm to be accounted for by standard PDR models. We propose a simple model, in which overlapping PDR clouds along the line of sight absorb the [OⅠ] 63 μm and [C Ⅱ] 158 μm emissions, and show that the proposed model reproduces the observed line intensities fairly well. In the σ Sco region, we have detected three fine-structure lines, [O Ⅰ] 63 μm, [N Ⅱ] 122 μm, and [C Ⅱ] 158 μm, and derived that 30%-80% of the [C Ⅱ] emission comes from the ionized gas. The upper limit of the [Si Ⅱ] 35 μm is compatible with the solar abundance relative to nitrogen, and no useful constraint on the gaseous Si is obtained for the a Sco region.
机译:我们已经在ISO上使用两个光谱仪(SWS和LWS)对ρOph和σSco星形成区域进行了一维光栅扫描观察。在ρOph区域中,检测到[SiⅡ] 35μm,[OⅠ] 63μm,146μm,[CⅡ] 15 8μm和H_2纯旋转过渡线S(0)至S(3),并根据太阳邻域值G_0〜30-500,气体密度n〜250-2500 cm〜(-3)和表面温度T〜100-400缩放辐射场,得出光解离区(PDR)特性。 K. [SiⅡ] 35μm与[OⅠ] 146μm的比率表明,太阳能PDR中10%-20%的硅必须呈气态,这表明即使在高温条件下,仍在进行有效的除尘。 PDR和一部分硅原子可能以挥发性形式包含在尘埃颗粒中。 [OⅠ] 63μm和[CⅡ] 158μm的发射相对于[OⅠ] 146μm来说太弱了,无法通过标准PDR模型进行解释。我们提出了一个简单的模型,在该模型中,沿视线重叠的PDR云吸收了[OⅠ] 63μm和[CⅡ] 158μm的发射,并表明该模型可以很好地再现观察到的线强度。在σSco区域中,我们检测到三条精细结构线,[OⅠ] 63μm,[NⅡ] 122μm和[CⅡ] 158μm,得出[CⅡ]的30%-80% ]发射来自电离气体。 [SiⅡ]35μm的上限与相对于氮的太阳丰度相适应,并且对于Sco区域没有获得对气态Si的有用限制。

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