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Chemical modeling of internal photon-dominated regions surrounding deeply embedded HC/UCH II regions

机译:深入嵌入HC / UCH II 区域周围的内部光子占主导区域的化学模型

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Aims. We aim to investigate the chemistry of internal photon-dominated regions (PDRs) surrounding deeply embedded hypercompact (HC) and ultracompact (UC) H II regions. We search for specific tracers of this evolutionary stage of massive star formation that can be detected with current astronomical facilities. Methods. We modeled hot cores with embedded HC/UCH II regions (called H II region models in the article despite the fact that we do not model the H II region itself), by coupling the astrochemical code Saptarsy to a radiative transfer framework obtaining the spatio-temporal evolution of abundances as well as time-dependent synthetic spectra. In these models where we focused on the internal PDR surrounding the H II region, the gas temperature is set to the dust temperature and we do not include dynamics thus the density structure is fixed. We compared this to hot molecular core (HMC) models and studied the effect on the chemistry of the radiation field which is included in the H II region models only during the computation of abundances. In addition, we investigated the chemical evolution of the gas surrounding H II regions with models of different densities at the ionization front, different sizes of the ionized cavity and different initial abundances. Results. We obtain the time evolution of synthetic spectra for a dozen of selected species as well as ratios of their integrated intensities. We find that some molecules such as C, N_(2)H~(+), CN, and HCO do not trace the inner core and so are not good tracers to distinguish the H II /PDR regions to the HMCs phase. On the contrary, C~(+)and O trace the internal PDRs, in the two models starting with different initial abundances, but are unfortunately currently unobservable with the current achievable spatial resolution because of the very thin internal PDR (Δ r _(PDR)< 100 AU). The emission of these two tracers is very dependent on the size of the H II region and on the density in the PDR. In addition, we find that the abundance profiles are highly affected by the choice of the initial abundances, hence the importance to properly define them.
机译:目的我们的目的是调查深埋的超紧凑(HC)和超紧凑(UC)H II区域周围的内部光子主导区域(PDR)的化学性质。我们寻找可以通过当前天文设施检测到的大规模恒星形成这一演化阶段的特定示踪剂。方法。我们通过将天化学代码Saptarsy与辐射转移框架耦合,获得了具有嵌入式HC / UCH II区域的热核模型(尽管我们并未对H II区域本身进行建模,但在本文中称为H II区域模型)。丰度的时间演变以及与时间有关的合成光谱。在这些模型中,我们关注H II区域周围的内部PDR,将气体温度设置为粉尘温度,并且不包含动力学,因此密度结构是固定的。我们将此与热分子核(HMC)模型进行了比较,并研究了仅在计算丰度期间对H II区模型中所包括的辐射场化学的影响。此外,我们用不同密度的电离前沿,不同大小的电离空腔和不同的初始丰度模型研究了H II区域周围气体的化学演化。结果。我们获得了十二种选定物种的合成光谱的时间演变及其综合强度的比率。我们发现某些分子,例如C,N_(2)H〜(+),CN和HCO不能追踪内核,因此也不是区分H II / PDR区域与HMCs相的良好示踪剂。相反,在两个模型中,C〜(+)和O跟踪内部PDR,它们以不同的初始丰度开始,但不幸的是,由于内部PDR非常薄,因此目前无法用当前可获得的空间分辨率观察到(Δr _(PDR )<100 AU)。这两种示踪剂的发射非常依赖于H II区的大小以及PDR中的密度。此外,我们发现,丰度曲线受初始丰度的选择的影响很大,因此正确定义它们的重要性。

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