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The giant H?ii region NGC 588 as a benchmark for 2D photoionisation models

机译:巨大的Hiiii地区NGC 588作为2D光电离模型的基准

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Aims. We use optical integral field spectroscopy and 8 μm and 24 μm mid-IR observations of the giant H?ii region NGC 588 in the disc of M33 as input and constraints for two-dimensional tailor-made photoionisation models under different geometrical approaches. We do this to explore the spatial distribution of gas and dust in the interstellar, ionised medium surrounding multiple massive stars. Methods. Two different geometrical approaches are followed for the modelling structure: i) Each spatial element of the emitting gas is studied individually using models, which assume that the ionisation structure is complete in each element, to look for azimuthal variations across gas and dust. ii) A single model is considered, and the two-dimensional structure of the gas and the dust are assumed to be due to the projection of an emitting sphere onto the sky. Results. The models in both assumptions reproduce the radial profiles of Hβ surface brightness, the observed number of ionising photons, and the strong optical emission-line relative intensities. The first approach produces a constant-density, matter-bounded thin shell of variable thickness and dust-to-gas ratio, while the second gives place to a radiation-bounded, thick shell sphere of decreasing particle density. However, the radial profile of the 8 μm/24 μm IR ratio, depending on the gas and dust geometry, only fits well when the thick-shell model is used. The resulting dust-to-gas mass ratio, which was obtained empirically from the derived dust mass using data from Spitzer, also has a better fit using the thick-shell solution. In both approaches, models support the importance of the low surface-brightness positions on the integrated spectrum of the nebula, the chemical homogeneity, the ionisation-parameter radial decrease, and the robustness of strong-line methods to derive the equivalent effective temperature in extended regions. These results must be taken with care in view of the very low extinction values that are derived from the IR, as compared to that derived from the Balmer decrement. Besides, the IR can be possibly contaminated with the emission from a cloud of diffuse gas and dust above the plane of the galaxy detected at 250 μm Herschel image.
机译:目的我们使用光学积分场光谱学和M33盘中巨大的H?ii区域NGC 588的8μm和24μm中红外观测作为输入和约束,以不同的几何方法进行二维量身定制的光电离模型。我们这样做是为了探索围绕多个大质量恒星的星际电离介质中气体和尘埃的空间分布。方法。对于建模结构,遵循两种不同的几何方法:i)使用模型分别研究发射气体的每个空间元素,这些模型假定每个元素中的电离结构都是完整的,以寻找气体和灰尘之间的方位角变化。 ii)考虑单个模型,并假定气体和粉尘的二维结构是由于发射球向天空的投影所致。结果。这两个假设中的模型都再现了Hβ表面亮度的径向分布,观察到的电离光子数以及较强的光发射线相对强度。第一种方法产生了厚度可变且粉尘与气体比率恒定的,受物质限制的薄壳,而第二种方法则产生了粒子密度递减的受辐射限制的厚壳球。但是,取决于气体和粉尘的几何形状,IR比率为8μm/ 24μm的径向轮廓仅在使用厚壳模型时才适合。使用Spitzer的数据从得出的粉尘质量凭经验获得的粉尘/气体质量比也可以通过厚壳解决方案更好地拟合。在这两种方法中,模型都支持在星云积分光谱上低表面亮度位置,化学均匀性,电离参数径向减小以及强线方法的稳健性的重要性,这些方法在扩展状态下得出等效有效温度地区。鉴于从IR得出的消光值与从Balmer减量得出的消光值相比非常低,因此必须谨慎考虑这些结果。此外,IR可能会被在250μmHerschel图像处检测到的银河平面上方的弥漫性气体和尘埃云的发射所污染。

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