论文标题
用HCO $^+$在化学上追踪原行星磁盘中的水雪线
Chemically tracing the water snowline in protoplanetary disks with HCO$^+$
论文作者
论文摘要
预计[删节]行星形成将在原月球磁盘中,尤其是水雪线周围的雪线周围增强。但是,水雪线与地球大气中的寄主恒星和水的近距离接近,这直接检测到质磁盘中的水雪线具有挑战性。在较早的Protostellar信封工作之后,这项研究的目的是研究Hco $^+$和H $^{13} $ CO $^+$的有效性,作为原行星磁盘的示踪剂,因为HCO $^+$被气相水破坏了。两个小型化学网络用于预测典型的Herbig AE磁盘中的HCO $^+$丰度。随后,对相应的排放配置文件进行了建模,以H $^{13} $ CO $^+$和HCO $^+$ $ J = 2-1 $建模,该$ $ $ $ J = 2-1 $,这在连续量排放的亮度和光学深度效果之间提供了最佳平衡。 HCO $^+$丰度在4.5 au的水雪线外面跳了两个数量级。我们发现H $^{13} $ co $^+$和HCO $^+$的排放是环形的三种效果:通过气相水,连续元素光学深度和分子激发效果破坏了HCO $^+$。气相水的存在导致磁盘中心的额外下降仅为$ \ sim $ 13%和24%,分别为H $^{13} $ CO $^+$和HCO $^+$。对于更加发光的爆发源V883ori,我们的模型预测,如果雪线位于$ \ sim $ 40 au之外,灰尘和激发的效果不会限制。我们对HCO $^+$ $ j = 3-2 $的ALMA观察结果的分析与位于100 au的水雪线一致。 HCO $^+$丰度在水雪线周围急剧下降,但是由于水雪线而导致的Hco $^+$排放的灰尘和激发可以掩盖Hco $^+$的下降。因此,在Herbig磁盘中使用HCO $^+$定位水雪线非常困难,但是爆发诸如V883ori之类的爆发可能是很困难的。
[Abridged] Planet formation is expected to be enhanced around snowlines in protoplanetary disks, in particular around the water snowline. However, the close proximity of the water snowline to the host star and water in the Earth's atmosphere makes a direct detection of the water snowline in protoplanetary disks challenging. Following earlier work on protostellar envelopes, the aim of this research is to investigate the validity of HCO$^+$ and H$^{13}$CO$^+$, as tracers of the water snowline in protoplanetary disks, as HCO$^+$ is destroyed by gas-phase water. Two small chemical networks are used to predict the HCO$^+$ abundance in a typical Herbig Ae disk. Subsequently, the corresponding emission profiles are modelled for H$^{13}$CO$^+$ and HCO$^+$ $J=2-1$, which provides the best balance between brightness and optical depth effects of the continuum emission. The HCO$^+$ abundance jumps by two orders of magnitude just outside the water snowline at 4.5 AU. We find that the emission of H$^{13}$CO$^+$ and HCO$^+$ is ring-shaped due to three effects: destruction of HCO$^+$ by gas-phase water, continuum optical depth, and molecular excitation effects. The presence of gas-phase water causes an additional drop of only $\sim$13% and 24% in the center of the disk, for H$^{13}$CO$^+$ and HCO$^+$, respectively. For the much more luminous outbursting source V883Ori, our models predict that the effect of dust and excitation are not limiting if the snowline is located outside $\sim$40 AU. Our analysis of ALMA observations of HCO$^+$ $J=3-2$ is consistent with the water snowline located around 100 AU. The HCO$^+$ abundance drops steeply around the water snowline, but dust and excitation can conceal the drop in HCO$^+$ emission due to the water snowline. Therefore, locating the water snowline with HCO$^+$ in Herbig disks is very difficult, but it is possible for outbursting sources like V883Ori.