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首页> 外文期刊>The Astrophysical journal >The Excitation and Metallicity of Galactic H II Regions from Infrared Space Observatory SWS Observations of Mid-Infrared Fine-Structure Lines*
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The Excitation and Metallicity of Galactic H II Regions from Infrared Space Observatory SWS Observations of Mid-Infrared Fine-Structure Lines*

机译:中红外精细结构线的红外空间天文台SWS观测对银河H II区的激发和金属性*

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We present mid-infrared Infrared Space Observatory Short-Wavelength Spectrometer (ISO-SWS) observations of the fine-structure emissions lines [Ne II] 12.8 μm, [Ne III] 15.6 μm, [Ne III] 36.0 μm, [Ar II] 6.99 μm, [Ar III] 8.99 μm, [S III] 18.7 μm, [S III] 33.5 μm, and [S IV] 10.5 μm and the recombination lines Brα and Brβ in a sample of 112 Galactic H II regions and 37 nearby extra-Galactic H II regions in the LMC, SMC, and M33. We selected our sources from archival ISO-SWS data as those showing prominent [Ne II] 12.8 μm or [Ne III] 15.6 μm emissions. The Galactic sources have a wide range in galactocentric distance (0 kpc Rgal 18 kpc), which enables us to study excitation and metallicity variations over large Galactic scales. We detect a steep rise in the [Ne III] 15.6 μm/[Ne II] 12.8 μm, [Ar III] 8.99 μm/[Ar II] 6.99 μm, and [S IV] 10.5 μm/[S III] 33.5 μm excitation ratios from the inner Galaxy outward, and a moderate decrease in metallicity, from ~2 Z☉ in the inner Galaxy to ~1 Z☉ in the outer disk. The extra-Galactic sources in our sample show low gas density, low metallicity, and high excitation. We find a good correlation between [Ne III] 15.6 μm/[Ne II] 12.8 μm and [Ar III] 8.99 μm/[Ar II] 6.99 μm excitation ratios in our sample. The observed correlation is well reproduced by theoretical nebular models that incorporate new-generation wind-driven non-LTE model stellar atmospheres for the photoionizing stars. In particular, the non-LTE atmospheres can account for the production of [Ne III] emission in the H II regions. We have computed self-consistent nebular and stellar atmosphere models for a range of metallicities (0.5-2 Z☉). We conclude that the increase in nebular excitation with galactocentric radius is due to an increase in stellar effective temperature (as opposed to a hardening of the stellar spectral energy distributions due to the metallicity gradient). We estimate an integrated [Ne III] 15.6 μm/[Ne II] 12.8 μm ratio for the Galaxy of 0.8, which puts it well inside the range of values for starburst galaxies. The good fit between observations and our models support the conclusion of Thornley and coworkers that the low [Ne III] 15.6 μm/[Ne II] 12.8 μm ratios observed in extra-Galactic sources are due to global aging effects.
机译:我们目前提供的中型红外空间天文台短波光谱仪(ISO-SWS)对精细结构发射线的观测值[Ne II] 12.8μm,[Ne III] 15.6μm,[Ne III] 36.0μm,[Ar II]在112个Galactic H II区域和37个附近的区域的样本中,重组线分别为6.99μm,[Ar III] 8.99μm,[S III] 18.7μm,[S III] 33.5μm和[S IV] 10.5μm,以及重组线Brα和Brβ LMC,SMC和M33中的银河外H II区。我们从档案ISO-SWS数据中选择了显示显着[Ne II] 12.8μm或[Ne III] 15.6μm排放的数据源。银河源的银心距离范围很广(0 kpc Rgal 18 kpc),这使我们能够研究大银河尺度上的激发和金属性变化。我们检测到[Ne III] 15.6μm/ [Ne II] 12.8μm,[Ar III] 8.99μm/ [Ar II] 6.99μm和[S IV] 10.5μm/ [S III] 33.5μm激增从内部银河向外的比率,以及金属性的适度降低,从内部银河的〜2Z☉到外盘的〜1Z☉。我们样本中的银河系外源显示出低气体密度,低金属性和高激发。我们在我们的样品中发现[Ne III] 15.6μm/ [Ne II] 12.8μm和[Ar III] 8.99μm/ [Ar II] 6.99μm激发比之间具有良好的相关性。理论上的星云模型很好地再现了观测到的相关性,该模型结合了新一代风驱动非LTE模型的恒星大气层,用于光电离恒星。尤其是,非LTE气氛可以解释H II区域中[Ne III]发射的产生。我们已经计算出了一系列金属性(0.5-2Z☉)的自洽星云和恒星大气模型。我们得出的结论是,星状中心半径的星云激发增加是由于恒星有效温度的升高(与之相反,由于金属度梯度使恒星光谱能量分布变硬)。我们估计星系的[Ne III] 15.6μm/ [Ne II] 12.8μm的综合比率为0.8,这使其处于星爆星系的数值范围之内。观测值与我们的模型之间的良好契合性支持Thornley及其同事得出的结论:银河系外源观测到的[Ne III] 15.6μm/ [Ne II] 12.8μm低比率是由于总体衰老效应所致。

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