论文标题

低积聚者的普查。 II:增生性能

A Census of the Low Accretors. II: Accretion Properties

论文作者

Thanathibodee, Thanawuth, Molina, Brandon, Serna, Javier, Calvet, Nuria, Hernández, Jesús, Muzerolle, James, Franco-Hernández, Ramiro

论文摘要

关于从原行星磁盘上吸收积聚到低质量预序列恒星(T Tauri恒星)的过程知之甚少。然而,目前尚不清楚积聚如何停止。为了确定积聚性能及其与恒星特性的关系并获得了对吸积的最后阶段的洞察力,我们提供了对24个低和可能的吸积的详细分析,以前使用He i $λ$ 10830行鉴定出来。我们使用磁层积聚流模型对这些恒星的中等分辨率H $α$曲线进行建模,这些模型解释了线中心的色球层贡献。基于可以与模型一起重现的20颗恒星拟合的参数,我们发现磁盘截断半径与质量积聚率与理论和模拟的预测一致的质量积聚率之间的幂律关系。比较旋转和截断半径,我们发现我们的大多数目标都在不稳定的制度中积聚,并排除螺旋桨作为停止积聚的主要过程。要使截断半径与磁性半径相同,偶极子磁场和/或效率参数$ξ$需要小于先前确定的,这表明高阶场在低积聚速率中占主导地位。最后,我们确定可通过H $α$线建模可以检测到的最低吸积率是$ 1-3 \ times10^{ - 11} m _ {\ odot} yr^{ - 1} $的M3星和$ 3-5 \ times10^{-11} M _ { - 11} M _ {\ odot} yr {\ odot}这些极限低于样品中观察到的积聚率,这表明我们已经达到了物理下限。此限制,$ \ dot {m} \ sim10^{ - 10} m _ {\ odot} yr^{ - 1} $,与euv为主的光蒸发一致。

Much is known about the processes driving accretion from protoplanetary disks onto low-mass pre-main-sequence stars (T Tauri stars). Nevertheless, it is unclear how accretion stops. To determine the accretion properties and their relation to stellar properties and gain insight into the last stages of accretion, we present a detailed analysis of 24 low and possible accretors, previously identified using the He I $λ$10830 line. We model moderate-resolution H$α$ profiles of these stars using magnetospheric accretion flow models that account for the chromospheric contribution at the line center. Based on parameters derived from the fits of 20 stars that can be reproduced with the models, we find a power-law relation between the disk truncation radius and the mass accretion rate consistent with predictions from theory and simulations. Comparing the corotation and truncation radii, we find that most of our targets are accreting in the unstable regime and rule out the propeller as the main process stopping accretion. For the truncation radius to be the same as the magnetic radius, the dipole magnetic field and/or the efficiency parameter $ξ$ need to be smaller than previously determined, suggesting that higher-order fields dominate in low accretion rates. Lastly, we determine that the lowest accretion rates that can be detected by H$α$ line modeling are $1-3\times10^{-11}M_{\odot}yr^{-1}$ for M3 stars and $3-5\times10^{-11}M_{\odot}yr^{-1}$ for K5 stars. These limits are lower than the observed accretion rates in our sample, suggesting that we have reached a physical lower limit. This limit, $\dot{M}\sim10^{-10}M_{\odot}yr^{-1}$, is consistent with EUV-dominated photoevaporation.

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