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Radiation thermo-chemical models of protoplanetary disks - II. Line diagnostics

机译:原行星盘的辐射热化学模型-II。线路诊断

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Aims. In this paper, we explore the diagnostic power of the far-IR fine-structure lines of [O I] 63.2m, 145.5m, [C II] 157.7m, as well as the radio and sub-mm lines of CO J=1-0,2-1 and 3-2 in application to disks around Herbig Ae stars. We aim atunderstanding where the lines originate from, how the line formationprocess is affected by density, temperature and chemical abundance inthe disk, and to what extent non-LTE effects are important. Theultimate aim is to provide a robust way to determine the gas mass ofprotoplanetary disks from line observations. Methods. We use the recently developed disk code P ROD IM Oto calculate the physico-chemical structure of protoplanetary disks andapply the Monte-Carlo line radiative transfer code R ATRAN to predict observable line profiles and fluxes. We consider a series of Herbig Ae type disk models ranging from 10-6to (between 0.5 and 700AU) to discuss the dependency of the linefluxes and ratios on disk mass for otherwise fixed disk parameters.This paper prepares for a more thorough multi-parameter analysisrelated to the Herschel open time key program G ASPS. Results. We find the [C II]157.7m line to originate in LTE from the surface layers of the disk, where .The total emission is dominated by surface area and hence depends strongly on disk outer radius. The [O I] lines can be very bright (>10-16W/m2) and form in slightly deeper and closer regions under non-LTE conditions. For low-mass models, the [O I]lines come preferentially from the central regions of the disk, and thepeak separation widens. The high-excitation [O I]145.5m line, which has a larger critical density, decreases more rapidly with disk mass than the 63.2m line. Therefore, the [O I] 63.2m/145.5m ratio is a promising disk mass indicator, especially as it is independent of disk outer radius for 200$ -->AU. CO is abundant only in deeper layers .For too low disk masses ()the dust starts to become transparent, and CO is almost completelyphoto-dissociated. For masses larger than that the lines are anexcellent independent tracer of disk outer radius and can break theouter radius degeneracy in the [O I]63.2m/[C II]157.7m line ratio. Conclusions. The far-IR fine-structure lines of [C II] and [O I]observable with Herschel provide a promising tool to measure the diskgas mass, although they are mainly generated in the atomic surfacelayers. In spatially unresolved observations, none of these lines carrymuch information about the inner, possibly hot regions <30AU. Key words: astrochemistry - methods: numerical - line: formation - circumstellar matter - stars: formation - radiative transfer
机译:目的在本文中,我们探讨了[OI] 63.2m,145.5m,[C II] 157.7m的远红外精细结构线以及CO J = 1的射电和亚毫米线的诊断能力-0,2-1和3-2适用于Herbig Ae星周围的磁盘。我们旨在了解线路的来源,磁盘中的密度,温度和化学丰度如何影响线路的形成过程,以及在何种程度上非LTE效应很重要。最终目的是提供一种从线观测确定原行星盘气体质量的可靠方法。方法。我们使用最近开发的磁盘代码P ROD IM O来计算原行星盘的物理化学结构,并应用蒙特卡洛线辐射传递代码R ATRAN来预测可观测的线轮廓和通量。我们考虑了一系列Herbig Ae型磁盘模型,范围从10-6到0.5至700AU之间,以讨论在其他固定磁盘参数下线通量和比率对磁盘质量的依赖性。本文为更全面的多参数分析做准备Herschel开放时间关键程序G ASPS。结果。我们发现[C II] 157.7m线起源于LTE,它来自磁盘的表层。总发射量由表面积决定,因此强烈依赖于磁盘的外半径。 [O I]线可能非常亮(> 10-16W / m2),并在非LTE条件下形成在更深和更近的区域。对于低质量模型,[O I]线优先来自磁盘的中心区域,并且峰间距增大。具有更大临界密度的高激发[O I] 145.5m线比63.2m线在磁盘质量方面的下降更快。因此,[O I] 63.2m / 145.5m的比值是一个很有前途的磁盘质量指标,特别是因为它与200 $-> AU的磁盘外半径无关。 CO仅在较深的层中富集。如果磁盘质量太低,灰尘开始变得透明,并且CO几乎完全被光解离。对于大于此质量的质量,这些线是磁盘外半径的出色独立跟踪器,并且可以打破[O I] 63.2m / [C II] 157.7m线比的外半径简并性。结论。用Herschel观察到的[C II]和[O I]的远红外精细结构线提供了一种有希望的工具来测量盘气质量,尽管它们主要在原子表面层中产生。在空间上无法分辨的观测中,这些线都没有携带有关内部(可能小于30AU)高温区域的大量信息。关键词:天化学-方法:数值-线:形成-绕星物质-恒星:形成-辐射转移

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